Method of Transmitting Energy Produced with Destructive Interference to a Target

ABSTRACT

Invention for efficiently transmitting energy to a target for producing an overall effective result for applications comprising power transmission and communications. Wherein, first, a source of electromagnetically intense coherent radiation and interferometric apparatus produce a beam of electromagnetically neutralized radiation. The neutralized beam comprises forward propagating photons or forward propagating electrically charged particles which comprise associated forward traveling transverse waves which superimpose and destructively interfere to an extent, and comprise associated oscillatorily time-varying electromagnetic fields which cancel to a corresponding extent. Then, second, the electromagnetically neutralized beam is coherently transmitted through transmission apparatus to a target. Wherein, the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the transmission apparatus, and the adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the destructive interference in, and the respective intensity eliminated from, the neutralized beam during transmission.

BACKGROUND OF THE INVENTION

1. Field of the Invention

In general, the present invention pertains to methods of transmitting energy. More specifically, the scope of the field of the present invention pertains to methods of transmitting energy for power transmission, and methods of transmitting energy in the form of signals for communications.

2. Prior Art of the Invention

In general, prior art pertinent to the present invention includes certain basic principles of the wave-particle duality of quantum mechanics. Wherein, in quantum mechanics, a beam of radiation (i.e., a beam of wave-particle behaving entities in quantum mechanically significantly large quantities such as, for example, a beam of propagating protons, a beam of propagating electrons, or a beam of quanta of electromagnetic radiation in quantum mechanically significantly large quantities) can electromagnetically interact with electrically charged particles comprised in a medium in which it is propagating in direct proportion to the time-averaged energy flux density (i.e., intensity) of the beam during propagation in the medium.

For the purposes of describing the present invention, a beam of radiation is considered to be totally electromagnetically neutralized when a beam comprises coherent forward traveling transverse waves which are superimposed totally out of phase so as to produce total destructive interference and total cancellation of associated electromagnetic fields. While, a beam of radiation is considered to be partly electromagnetically neutralized when a beam comprises coherent forward traveling transverse waves which are superimposed partly out of phase so as to produce partial destructive interference and partial constructive interference, and so as to produce partial cancellation and partial reinforcement of associated electromagnetic fields. Wherein, electromagnetic interaction of a beam of electromagnetically neutralized radiation with electrically charged particles comprised in a medium in which it is propagating is eliminated in direct proportion to the destructive interference in, and the corresponding time-averaged energy flux density which is eliminated from, the neutralized beam during transmission in the medium. (Note that electromagnetic neutralization of a beam includes the electric charge neutralization of electrically charged particles in the electromagnetically neutralized beam in direct proportion to the corresponding electromagnetic neutralization of the beam when a beam of electromagnetically neutralized electrically charged particles is applied.)

More specific prior art pertinent to the present invention includes, for example, prior art which applies an interferometric system comprising a source of forward propagating intense radiation and interferometric apparatus in order to “eliminate energy” from the respective prior art system (e.g., prior art which applies an anti-reflecting thin film system in order to eliminate glare or, in general, back reflections from the prior art system). In contrast, the present invention applies a source of electromagnetically intense coherent forward propagating radiation and interferometric apparatus for producing a beam of electromagnetically neutralized radiation which is applied for transmitting energy (per se) from one location to another location (i.e., to a target) in an energy efficient manner (i.e., while conserving energy), and then the transmitted energy is subsequently utilized to produce a result in an overall effective manner.

In some generalized preferred embodiments in which the present invention is applied for the transmission and subsequent utilization of energy in an effective manner, apparatus provided, which comprises a source of electromagnetically intense coherent forward propagating radiation and interferometric apparatus, produces a beam of electromagnetically neutralized radiation which is, then, coherently transmitted by transmission apparatus to a target comprising a utilization apparatus. In which case, the adverse electromagnetic interaction of the electromagnetically neutralized beam with electrically charged particles comprised in the coherent transmission apparatus is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission, such that the adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated. Then, energy is transferred from the transmitted beam to the utilization apparatus in order to produce a result.

Prior art pertinent to the present invention for power transmission includes electrical power transmission systems which apply electrical conductors (e.g., copper wire, copper cable, or superconductors) for conducting electricity for power. Wherein, copper wire or cable related prior art systems have disadvantages which include energy inefficiency due to power attenuation. In particular, copper cable related prior art power transmission systems have disadvantages which include energy inefficiency due to transmission loss, dangerously high electrical voltages associated with relatively high voltage power lines, adverse antenna-based effects (including the production of extra low frequency, i.e., ELF, electric and magnetic fields; and interference effects), and have the disadvantage of a relatively high cost as pertains to, for example, the cost of the application of copper cable of relatively high purity and the cost of insulation. While, superconductors require relatively high amounts of energy for cooling in order to transmit energy for power in a relatively high energy efficient manner.

The application of the present invention for power transmission applies a method which produces a beam of electromagnetically neutralized radiation which is then coherently transmitted to a power utilization apparatus without the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the coherent transmission medium (e.g., coherently transmitting air filled tubing) in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission. Wherein, the adverse electromagnetic effects of transmitting energy for power such as energy inefficiency due to power attenuation, relatively high voltages, and certain adverse antenna-based effects (as aforementioned with respect to the prior art) are decreased with the application of the method of the present invention. While furthermore, the high cost of making a power conveying medium is also considered to be decreased with the application of the method of the present invention by, for example, applying air filled tubing instead of copper cables and superconductors as applied in respectively related prior art power transmission systems. Nevertheless, the present invention provides for a form of electromagnetically “resistance-less” or “low-resistance” power transmission depending upon if the applied beam of electromagnetically neutralized radiation is totally or partly electromagnetically neutralized, respectively.

Prior art pertinent to the present invention for wireline communications includes copper wire, coaxial cable, and fiber optic communications systems. Wherein, such prior art communications systems have disadvantages which include: a) energy inefficiency due to signal attenuation by a transmitting medium which disadvantageously causes the unnecessary need for relatively high power transmitter output and/or the need for unnecessary signal amplification (or repeating); b) the exclusion of bandwidth in terms of frequencies due to signal attenuation by the transmitting medium; c) a loss of bandwidth due to relatively slow signal propagation speed, which in the case of an optical fiber, for example, is due to a relatively high refractive index of an optical fiber compared to the air filled tubing which is applied as the transmitting medium in some preferred embodiments the present invention; and, with respect to fiber optics communications systems in particular, d) the relative high cost of making and deploying optical fibers.

The application of the present invention for wireline communications applies a data encoded beam of electromagnetically neutralized quanta of electromagnetic radiation which is coherently transmitted to a receiver without the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the coherent transmission medium (e.g., air filled tubing or optical fiber) in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission. Wherein, the adverse electromagnetic effects of transmitting data for wireline communications are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

In which case, for example, signal attenuation is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the coherently transmitted beam of electromagnetically neutralized quanta of electromagnetic radiation during transmission so as to increase the distance a signal can travel without being amplified (or repeated), such that the need for relatively high transmitter power output and/or the need for signal amplification (or repeating) is eliminated to a directly proportional extent, and such that the bandwidth (in terms of frequencies) which is available for signal transmission is increased. While also, the refractive index of the transmitting medium can be decreased with the application of air filled tubing as the transmitting medium relative to, in particular, an optical fiber, such that the speed at which a signal travels can be increased, and therefore the bandwidth (in terms of the speed of data transmission) can be increased. While, moreover, the present invention is considered to eliminate some of the cost of making and deploying a conveying medium for high bandwidth data transmission in wireline communications in preferred embodiments where air filled tubing is applied instead of, for example, optical fiber, and thus eliminate complications in, for example, the so called “last mile problem.”

Other prior art pertinent to the present invention for communications includes wireless communications systems for transmitting electromagnetic radiation for data transmission. Wherein, such prior art communications systems have disadvantages which include energy inefficiency due to signal attenuation which disadvantageously causes the unnecessary need for relatively high power transmitter output and/or the need for unnecessary signal amplification (or repeating), and thus also disadvantageously excludes bandwidth (in terms of frequencies) due to signal attenuation by the transmitting medium, i.e., by the air.

The application of the present invention for wireless communications applies a data encoded beam of electromagnetically neutralized quanta of electromagnetic radiation which is coherently transmitted to a receiver without the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the coherent transmission medium, which includes air, in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission. Wherein, the adverse electromagnetic effects of transmitting data for wireless communications are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated, e.g., signal attenuation is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the coherently transmitted beam of electromagnetically neutralized quanta of electromagnetic radiation during transmission so as to increase the distance a signal can travel without being amplified (or repeated), such that the need for relatively high transmitter power output and/or the need for signal amplification (or repeating) is eliminated to a directly proportional extent, and such that the bandwidth (in terms of frequencies) which is available for signal transmission is increased.

SUMMARY OF THE INVENTION

In general, the present invention is applied for coherently transmitting electromagnetically neutralized radiation, which is produced with destructive interference, in an energy efficient manner to a target which utilizes the transmitted energy to produce a result. The present invention is applied in general as follows:

Step 1) Providing a source of electromagnetically intense coherent forward propagating radiation and interferometric apparatus (e.g., a version of a Michelson interferometric apparatus) for producing a beam of electromagnetically neutralized radiation comprising coherent forward propagating radiation (in quantum mechanically significantly large quantities) which comprises forward propagating photons, or forward propagating electrically charged particles of the same sort, e.g., forward propagating electrons. Wherein, the forward propagating radiation comprises forward traveling transverse waves which destructively interfere to an extent, and associated electromagnetic fields which cancel to a corresponding extent;

Step 2) Coherently transmitting the beam of electromagnetically neutralized radiation in an energy efficient manner through coherent transmission apparatus to a target. In which case, the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the transmission apparatus, and the adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the destructive interference in, and the corresponding time-averaged energy flux density which is eliminated from, the electromagnetically neutralized beam during transmission. (Note that electromagnetic neutralization of a beam includes the electric charge neutralization of electrically charged particles in the electromagnetically neutralized beam in direct proportion to the corresponding electromagnetic neutralization of the beam when a beam of electromagnetically neutralized electrically charged particles is applied.); and

Step 3) Energy is transferred from the transmitted beam to a utilization apparatus comprised in the target in order to produce a result.

Some generalized preferred embodiments are applied for the transmission and subsequent utilization of energy in an effective manner. Wherein, in each such embodiment, apparatus provided, which comprises a source of electromagnetically intense coherent forward propagating radiation and interferometric apparatus, produces a beam of electromagnetically neutralized radiation which is then coherently transmitted by coherent transmission apparatus to a target comprising a utilization apparatus. In which case, the adverse electromagnetic interaction of the neutralized beam with electrically charged particles in the transmission apparatus is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission, such that the adverse electromagnetic effects of transmitting energy are eliminated to a directly proportional extent.

Then, energy is transferred from the transmitted beam to the utilization apparatus in order to produce a result by a utilization process which comprises one of the following examples depending on the embodiment applied:

1a) a momentum-based utilization process in which apparatus comprising, for example, a pressure transducer utilizes pressure applied by a transmitted electromagnetically neutralized particle beam in order to produce electrical voltage, e.g., for supplying power to a load, or for providing retrievable data for communications when the momentum comprised by the neutralized particle beam is modulated so as to encode data; or 1b) the momentum-based utilization process can be repeated by reflecting the transmitted electromagnetically neutralized particle beam, and then coherently transmitting the neutralized beam to at least one other pressure transducer and/or back to the first pressure transducer, and then utilizing the neutralized beam at least one more time in order to produce a plurality of electrical voltages for supplying more power to one load, or for supplying power to more than one load; or, still yet, the momentum-based utilization process can be repeated as such in order to provide data which can be retrieved over an interval of time when the momentum comprised by the neutralized particle beam is modulated so as to encode data in order that the momentum comprised by the neutralized particle beam is utilized, for example, for data buffering or data caching;

2) an electromagnetic-based utilization process in which apparatus utilizes a transmitted beam of partly electromagnetically neutralized radiation when a beam of partly electromagnetically neutralized radiation is applied, e.g., a process in which a photodetector or a particle detector utilizes a transmitted beam of partly electromagnetically neutralized radiation in order to produce electrical output for photon or electrically charged particle detection, respectively; or

3) a utilization process in which the target incoherently scatters a transmitted electromagnetically neutralized beam so as to produce a beam of electromagnetically intense radiation comprising incoherent radiation which is utilized in due course by an electromagnetic-based utilization apparatus to produce a result, e.g., a process in which a photodetector or a particle detector utilizes the electromagnetically intense beam in order to produce electrical output for photon or electrically charged particle detection, respectively (wherein the utilizing apparatus also utilizes any transmitted remaining portion of a beam of partly electromagnetically neutralized radiation which is not incoherently scattered if a beam of partly electromagnetically neutralized radiation is applied).

Other generalized preferred embodiments of the present invention are different by applying a filtering apparatus to eliminate any unwanted electromagnetically intense radiation which may be produced by systematic and/or random error from an applied beam of electromagnetically neutralized radiation. While, yet other generalized preferred embodiments apply shielding apparatus in whole, or in part, around an embodiment in order to shield the environment from electromagnetically neutralized and/or electromagnetically intense radiation which travels beyond a desired boundary around an embodiment of the present invention.

Other preferred embodiments describe different ways of adjusting the present invention in order to effectively accomplish the result of an application of the present invention. Such embodiments include an embodiment which describes time-averaged particle flux density adjustment, embodiments which describe time-averaged energy flux density adjustments, and an embodiment which describes focal point depth positioning adjustment.

More specific preferred embodiments are applied for the transmission and subsequent utilization of power (per se) in an effective manner. Wherein, in each such embodiment, apparatus provided, which comprises a source of electromagnetically intense coherent forward propagating radiation and interferometric apparatus, produces a beam of electromagnetically neutralized radiation which is then coherently transmitted by a coherent transmission medium, which includes air filled tubing, to a target comprising a power utilization apparatus. In which case, the adverse electromagnetic interaction of the neutralized beam with electrically charged particles in the air filled tubing is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission, such that the adverse electromagnetic effects of transmitting energy for power (e.g., power attenuation) are eliminated to a directly proportional extent.

Then, energy is transferred from the transmitted beam to the utilization apparatus in order to produce a result by a power utilization process which includes one of the following examples depending upon the embodiment applied: a) a momentum-based utilization process in which apparatus comprising, for example, a pressure transducer utilizes pressure applied by a transmitted electromagnetically neutralized particle beam in order to produce electrical voltage for supplying power to a load; b) an electromagnetic-based utilization process in which apparatus utilizes the power of a transmitted beam of partly electromagnetically neutralized radiation, e.g., a photodetector utilizes a transmitted beam of partly electromagnetically neutralized quanta of electromagnetic radiation in order to produce electrical output for supplying power to a load (when a partly electromagnetically neutralized beam is applied); or c) a utilization process in which the target incoherently scatters a transmitted beam of electromagnetically neutralized radiation so as to produce a beam of electromagnetically intense radiation comprising incoherent radiation, e.g., incoherent quanta of electromagnetic radiation, which is utilized in due course by an electromagnetic-based utilization apparatus, e.g., a photodetector, to produce electrical output for supplying power to a load, i.e., utilizes the respectively produced incoherent beam, or also utilizes any transmitted remaining portion of a beam of partly electromagnetically neutralized radiation which is not incoherently scattered if a beam of partly electromagnetically neutralized radiation is applied.

Other more specific preferred embodiments are applied for the transmission and subsequent utilization of data in an effective manner for wireline communications. Wherein, in each such embodiment, apparatus provided, which comprises a miniature laser and interferometric apparatus, produces a modulated beam of electromagnetically neutralized quanta of electromagnetic radiation which is then coherently transmitted by a coherent transmission medium, which includes air filled tubing or optical fiber, to a receiver which then utilizes the data encoded in the modulated beam for communications by a method which applies one of the power utilization processes which were previously described for embodiments which transmit and subsequently utilize power (per se) except that the data encoded in the power of the transmitted neutralized beam is utilized by the receiver for communications. Nevertheless, the adverse electromagnetic interaction of the coherently transmitted beam of electromagnetically neutralized quanta of electromagnetic radiation with electrically charged particles in the air filled tubing or the optical fiber is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission, such that the adverse electromagnetic effects of transmitting energy for wireline communications are eliminated to a directly proportional extent. In which case, for example, signal attenuation is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the beam of electromagnetically neutralized quanta of electromagnetic radiation during transmission so as to increase the distance a signal can travel without being amplified (or repeated), such that the need for relatively high transmitter power output and/or the need for signal amplification (or repeating) is eliminated to a directly proportional extent, and such that the bandwidth (in terms of frequencies) which is available for signal transmission is increased. While also, the refractive index of the transmitting medium can be decreased with the application of air filled tubing relative to, in particular, an optical fiber, such that the speed at which a signal travels can be increased, and therefore the bandwidth (in terms of the speed of data transmission) can be correspondingly increased. While, moreover, the complexities of making and deploying a conveying medium for high bandwidth data transmission for wireline communications can be eliminated to an extent by applying air filled tubing instead of optical fiber.

Still other more specific preferred embodiments of the present invention combine the uses of the present invention for power and wireline communications. In which case, such embodiments each employ a method which is applied for transmitting a modulated beam of electromagnetically neutralized radiation along air filled tubing or optical fiber to a target which then utilizes the power in the transmitted beam for both power per se as a utility, and for the data encoded in the power of the transmitted beam for communications.

While, yet still other more specific preferred embodiments are applied for wireless communications in an effective manner, and are different from the previously described preferred embodiments which are applied for wireline communications in that each applies a method which includes the coherent transmission of a beam of electromagnetically neutralized quanta of electromagnetic radiation through air instead of air filled tubing or optical fiber. Wherein, in each such embodiment, the adverse electromagnetic interaction of a beam of electromagnetically neutralized quanta of electromagnetic radiation with electrically charged particles in the air is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission, such that the adverse electromagnetic effects of transmitting energy for wireless communications are eliminated to a directly proportional extent, e.g., signal attenuation is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the beam of electromagnetically neutralized quanta of electromagnetic radiation during transmission so as to increase the distance a signal can travel without being amplified (or repeated), such that the need for relatively high transmitter power output and/or the need for signal amplification (or repeating) is eliminated to a directly proportional extent, and such that the bandwidth (in terms of frequencies) which is available for signal transmission is increased.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. (1) illustrates a side view of a generalized drawing of a preferred embodiment of the present invention which is applied for transmitting energy in an energy efficient manner in which a beam of electromagnetically neutralized radiation is applied.

FIG. (1′) is a top view of a somewhat detailed illustration of one version of the preferred embodiment illustrated in FIG. (1), and especially illustrates apparatus (2′) (comprising a version of a Michelson interferometric apparatus) which is one version of apparatus (2) which is illustrated in FIG. (1).

FIG. (2) illustrates a side view of a somewhat generalized preferred embodiment of the present invention which is applied for transmitting energy in an energy efficient manner, and is more specific than the preferred embodiment illustrated in FIG. (1) by applying a beam of totally electromagnetically neutralized radiation.

FIG. (2-a) illustrates the construction of a beam of totally electromagnetically neutralized radiation which is one version of the beam of totally electromagnetically neutralized radiation illustrated in FIG. (2).

FIG. (2-b) illustrates a pulsed beam of totally electromagnetically neutralized radiation which is another version of the beam of totally electromagnetically neutralized radiation illustrated in FIG. (2).

FIG. (2-c) illustrates an amplitude modulated pulsed beam of totally electromagnetically neutralized radiation which digitally encodes data, and is yet another version of the beam of totally electromagnetically neutralized radiation illustrated in FIG. (2).

FIG. (3) illustrates a side view of another somewhat generalized preferred embodiment of the present invention which is applied for transmitting energy in an energy efficient manner, and is more specific than the preferred embodiment illustrated in FIG. (1) by applying a beam of partly electromagnetically neutralized radiation.

FIG. (3-a) illustrates the construction of a beam of partly electromagnetically neutralized radiation which is one version of the beam of partly electromagnetically neutralized radiation illustrated in FIG. (3).

FIG. (3-b) illustrates a pulsed beam of partly electromagnetically neutralized radiation which is another version of the beam of partly electromagnetically neutralized radiation illustrated in FIG. (3).

FIG. (3-c) illustrates an amplitude modulated pulsed beam of partly electromagnetically neutralized radiation which digitally encodes data, and is yet another version of the beam of partly electromagnetically neutralized radiation illustrated in FIG. (3).

FIG. (4) illustrates a side view of one generalized preferred embodiment of the present invention which is applied for the transmission and subsequent utilization of energy in an effective manner, in which case the momentum comprised by a transmitted electromagnetically neutralized particle beam is utilized by a momentum-based utilizing apparatus (e.g., a pressure transducer) comprised in a target.

FIG. (5) illustrates a side view of another generalized preferred embodiment which is applied for the transmission and subsequent utilization of energy in an effective manner, in which case a transmitted beam of partly electromagnetically neutralized radiation is utilized by an electromagnetic-based utilizing apparatus (e.g., a photodetector or a particle detector) comprised in a target.

FIG. (6) illustrates a side view of a generalized conditional preferred embodiment which is applied for the transmission and subsequent utilization of energy in an effective manner, in which case certain steps are applied depending upon the beam of electromagnetically neutralized radiation which is applied, and depending upon the incoherently scattering apparatus which is (or are) applied in the target.

FIG. (7) illustrates a side view of another generalized preferred embodiment which is applied for the transmission and subsequent utilization of energy in an effective manner which is different by applying a beam of electromagnetically neutralized radiation, and combining incoherently scattering and transmitting apparatus with electromagnetic-based utilizing apparatus into one apparatus in the target.

FIGS. (8 a) and (8 b) illustrate side views of two embodiments of the present invention which together represent one aspect of the significance of adjusting the time-averaged particle flux density of a beam of electromagnetically neutralized radiation applied in the present invention.

FIGS. (9 a) and (9 b) illustrate side views of two embodiments of the present invention which together represent one aspect of the lack of the significance of adjusting the time-averaged energy flux density of a beam of electromagnetically neutralized radiation applied in the present invention.

FIGS. (10 a) and (10 b) illustrate side views of two embodiments of the present invention which together represent one aspect of the significance of adjusting the time-averaged energy flux density of a beam of electromagnetically neutralized radiation applied in the present invention.

FIGS. (11 a) and (11 b) illustrate side views of two embodiments of the present invention which together represent one aspect of the significance of adjusting the depth of the focal point of a beam of electromagnetically neutralized radiation in an incoherently scattering and transmitting target apparatus applied in the present invention.

FIG. (12 a) is an illustration of a side view of a somewhat specific preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and includes a longitudinally sectioned view of the respectively applied air filled tubing.

FIG. (12 b) is an illustration of a side view of a somewhat different preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and also includes a longitudinally sectioned view of the respectively applied air filled tubing, and is different by applying air filled tubing as a splitter.

FIG. (12 c) is an illustration of a side view of another somewhat different preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and also includes a longitudinally sectioned view of the respectively applied air filled tubing, and is different by applying air filled tubing as a coupler.

FIG. (12 d) is an illustration of a side view of yet another somewhat different preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and also includes a longitudinally sectioned view of the respectively applied air filled tubing, and is different by applying air filled tubing as a splitter and a coupler.

FIG. (13) is an illustration of a side view of a somewhat specific preferred embodiment of the present invention which is applied for transmitting data in an effective manner for wireline communications, and includes a longitudinally sectioned view of the air filled tubing which is respectively applied for data transmission.

FIG. (14) illustrates a side view of another somewhat specific preferred embodiment of the present invention which is applied for transmitting data in an effective manner for wireline communications which is different by applying wave division multiplexing and demultiplexing.

FIG. (14′) illustrates a side view of yet another somewhat specific preferred embodiment which is applied for transmitting data in an effective manner for wireline communications which is a more specific version of the preferred embodiment illustrated in FIG. (14) by applying a prism as a multiplexer and a prism as a demultiplexer in a wave division multiplexing and demultiplexing method of wireline communications.

FIG. (15) illustrates a somewhat specific preferred embodiment of the present invention which is applied for transmitting data in an effective manner for wireless communications which is different from certain embodiments for wireline communications (including the preferred embodiment illustrated in FIG. 13) by applying a method which includes the application of air as a coherent transmission medium instead of air filled tubing.

FIG. (16) illustrates a side view of another somewhat specific preferred embodiment of the present invention which is applied for transmitting data in an effective manner for wireless communications which is different from certain embodiments for wireline communications (including the preferred embodiment illustrated in FIG. 14) by applying a method of wave division multiplexing and demultiplexing which applies air as a coherent transmission medium instead of air filled tubing.

DETAILED DESCRIPTION OF THE INVENTION

First, certain general modes of operating the present invention are described in some generalized preferred embodiments which include descriptions of some ways certain embodiments of the present invention can be adjusted in order to accomplish their overall objectives in an effective manner. Then, certain more specific modes of operating the present invention are described in some more specific preferred embodiments for applications comprising power transmission and communications. (Refer to the notes at the end of this detailed description for the clarification of certain terms applied herein.)

FIG. (1) illustrates a side view of a generalized preferred embodiment of the present invention (illustrated in a general way by block drawing) which is applied for efficiently transmitting energy (per se) from one location to another location where there is a target which subsequently utilizes the transmitted energy to produce a result in an overall effective manner. The preferred embodiment illustrated in FIG. (1) is applied as follows:

Step 1) Apparatus (2), comprising a source of electromagnetically intense coherent forward propagating radiation (e.g., a laser) and interferometric apparatus (e.g., a version of a Michelson interferometric apparatus as illustrated in FIG. 1′), produces a beam of electromagnetically neutralized radiation (4). Beam (4) comprises, as examples, a beam of electromagnetically neutralized quanta of electromagnetic radiation (comprising photons), or a beam of electromagnetically neutralized electrically charged particles of the same sort, e.g., a beam of electromagnetically neutralized electrons.

More specifically, the beam of electromagnetically neutralized radiation (4) comprises coherent forward propagating radiation which comprises wave-particle behaving entities (in quantum mechanically significantly large quantities) which each comprise a forward traveling transverse wave with an associated oscillatorily time-varying electromagnetic field, total energy, and momentum. Wherein, the waves comprised in beam (4) are superimposed out of phase to an extent so that the displacement vectors of the waves in the beam cancel in direct proportion to the extent to which the waves are out of phase, and so that the waves destructively interfere, and the associated electromagnetic fields cancel, to a corresponding extent.

Note that a beam of electromagnetically neutralized radiation can comprise a beam of totally electromagnetically neutralized radiation which is produced with total destructive interference of waves and total cancellation of associated electromagnetic fields, such that the beam is totally electromagnetically neutralized in agreement with the total elimination of time-averaged energy flux density from the beam, as relates to certain preferred embodiments which follow including the preferred embodiment illustrated in FIG. (2); or a beam of electromagnetically neutralized radiation can comprise a beam of partly electromagnetically neutralized radiation which is produced with partial destructive interference of waves and partial cancellation of associated electromagnetic fields, such that a beam of partly electromagnetically neutralized radiation is electromagnetically neutralized in direct proportion to the time-averaged energy flux density which is eliminated from the partly neutralized beam, as relates to certain preferred embodiments which follow including the preferred embodiment illustrated in FIG. (3). Also, note that electromagnetic neutralization of the beam includes the electric charge neutralization of electrically charged particles in the electromagnetically neutralized beam in direct proportion to the corresponding electromagnetic neutralization of the beam when a beam of electromagnetically neutralized electrically charged particles is applied;

Step 2) From apparatus (2), the beam of electromagnetically neutralized radiation (4) is coherently transmitted by coherent transmission apparatus (6) to target (8). Here, again, during coherent transmission by apparatus (6) to target (8), beam (4) comprises forward traveling transverse waves which are superimposed out of phase to an extent so as to produce destructive interference to an extent, such that the associated electromagnetic fields in beam (4) cancel to a corresponding extent.

In effect, the adverse electromagnetic interaction of electromagnetically neutralized beam (4) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6) is eliminated in direct proportion to the destructive interference in, and the corresponding time-averaged energy flux density which is eliminated from, beam (4) during transmission. Wherein, the adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated; and

Step 3) Energy is transferred from the transmitted beam to a utilization apparatus comprising a transducer which is comprised in the target in order to produce a result.

Note that an electromagnetically intense entity comprised in coherent transmission apparatus (6) can comprise: a) a static electrically charged particle, e.g., a static proton or a static electron; b) an electron in an orbital of an atom or a molecule; c) a freely propagating electrically charged particle (on average over time), e.g., an electron or proton which is propagating by itself (on average over time), or an electron or a proton which is propagating in a beam of electrically charged particles comprising a non-zero magnitude of time-averaged energy flux density; or, exclusively for the application of a beam of electromagnetically neutralized electrically charged particles, an electromagnetically intense entity can comprise d) a quantum of electromagnetic radiation, e.g., a quantum of electromagnetic radiation which is propagating by itself (on average over time), or a quantum of electromagnetic radiation comprised in a beam of quanta of electromagnetic radiation which comprises a non-zero magnitude of time-averaged energy flux density. Also, note that a given beam of electromagnetically neutralized radiation also comprises a time-averaged particle flux density which can be calculated by the quantization of the momentum of the given electromagnetically neutralized beam which can be measured, for example, by pressure detection; or calculated by the quantization of the time-averaged energy flux density of a hypothetical beam of radiation which is equivalent to the given beam of electromagnetically neutralized radiation except that the respectively comprised waves are totally in phase so as to produce total constructive interference and total reinforcement of the associated oscillatorily time-varying electromagnetic fields. Wherein, in the latter case, the measurement of the time-averaged energy flux density of the hypothetical beam is accomplished by way of electromagnetic interaction. Moreover, note that radiation comprised in the neutralized beam comprises “particles” (e.g., photons or electrons) which are associated with the waves, wherein the waves experience superposition and interference, not the particles, and the radiation is not destroyed by destructive interference in agreement with the laws of the conservation of energy and momentum.

FIG. (1′) is a somewhat detailed illustration of one version of the preferred embodiment illustrated in FIG. (1). Wherein, apparatus (2′), which is a top view of one version of apparatus (2) (which is illustrated in FIG. 1), comprises a version of a Michelson interferometric apparatus.

In which case, in FIG. (1′), source (3), e.g., a laser, produces a beam of electromagnetically intense coherent forward propagating radiation, e.g., a collimated laser beam, which is coherently transmitted by the air (6′) to a plane beam splitter (7) (e.g., a partly transmitting and partly reflecting mirror), and then is divided (i.e., partly transmitted and partly reflected) by beam splitter (7) so as to produce a first transmitted intense coherent beam fraction and a first reflected intense coherent beam fraction. Then, the first transmitted beam fraction is coherently transmitted by the air (6′) to the totally reflecting retroreflector (9), and the first reflected beam fraction is transmitted by the air (6′) to the totally reflecting retroreflector (11). Then, retroreflector (9) totally reflects the first transmitted beam fraction in a coherent manner so that the first transmitted beam fraction is then coherently transmitted by the air (6′) back to beam splitter (7), which then divides the first transmitted beam fraction so as to produce a second transmitted intense coherent beam fraction which is transmitted towards absorber (13), and so as to also produce a second reflected intense coherent beam fraction which is reflected in a coherent manner towards target (8′). Also, retroreflector (11) totally reflects the first reflected beam fraction in a coherent manner so that the first reflected beam fraction is then coherently transmitted by the air (6′) back to beam splitter (7) which then divides the first reflected beam fraction so as to produce a third transmitted intense coherent beam fraction which is transmitted towards target (8′), and so as to also produce a third reflected intense coherent beam fraction which is reflected towards absorber (13).

Wherein, the second reflected intense coherent beam fraction and the third transmitted intense coherent beam fraction combine at splitter (7) after traveling different path lengths, such that the forward traveling transverse waves comprised by these combined beam fractions superimpose out of phase to an extent so as to produce destructive interference to an extent, and such that the associated electric and magnetic fields comprised in these combined beam fractions each cancel to a corresponding extent. Thus, the second reflected beam fraction and the third transmitted beam fraction combine to produce a beam of electromagnetically neutralized radiation (4′). (Also, similarly, the second transmitted beam fraction and the third reflected beam fraction combine at beam splitter 7 so as to produce an extraneous beam of electromagnetically neutralized radiation which is transmitted to absorber 13. Note that absorber 13 can absorb the extraneous beam of electromagnetically neutralized radiation by incoherently scattering the extraneous beam with incoherently scattering apparatus so as to produce electromagnetically intense radiation, and, in due course, electromagnetically absorbing the electromagnetically intense radiation thereby produced with absorptive apparatus by way of electromagnetic interaction.)

Next, the beam of electromagnetically neutralized radiation (4′) is coherently transmitted by the air (6′) to coherent transmission apparatus (6″), e.g., air. Then, finally, electromagnetically neutralized beam (4′) is coherent transmitted by coherent transmission apparatus (6″) to target (8′).

Wherein, the adverse electromagnetic interaction of neutralized beam (4′) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6″) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4′) during transmission in apparatus (6″). While, the adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

FIG. (2) illustrates a side view of a somewhat more specific preferred embodiment which is applied for transmitting energy in an energy efficient manner. Steps 1) and 2) applied in the preferred embodiment which pertains to FIG. (1) are, in general, applicable in the preferred embodiment illustrated in FIG. (2) except that, more specifically, apparatus (2 a) produces a beam of totally electromagnetically neutralized radiation (4 a) which is coherently transmitted by coherent transmission apparatus (6 a) to target (8 a). In effect, the adverse electromagnetic interaction of neutralized beam (4 a) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 a) is totally eliminated in direct proportion to (in agreement with) the total electromagnetic neutralization of beam (4 a) during transmission. Wherein, the adverse electromagnetic effects of transmitting energy are totally eliminated.

In the preferred embodiment illustrated in FIG. (2), coherent transmission processes involve potential-energy-based coherent transmission processes which include a quantum mechanical functional relation between the total energy comprised by the coherently transmitted electromagnetically neutralized radiation in beam (4 a) and the potential energy comprised by coherent transmission apparatus (6 a). (Refer to the preferred embodiment for power transmission which pertains to FIG. 12 a, and the preferred embodiment which applies an optical fiber for wireline communications, for some details of some of the parameters of some example potential-energy-based coherent transmission media.)

FIG. (2-a) illustrates the construction of a beam of totally electromagnetically neutralized radiation (4 b) which is one version of beam (4 a) (illustrated in FIG. 2). Wherein, FIG. (2-a) illustrates intense coherent beam portions of radiation (10 b) and (12 b) which are aligned parallel to the given (t) axis along the directions of propagation (14 b) and (20 b), respectively. Beam portions (10 b) and (12 b) comprise the linearly polarized sinusoidally time-varying forward traveling transverse wave components (16 b) and (22 b), respectively, which are linearly polarized in the (t-y) plane, and are each associated with a respective linearly polarized sinusoidally time-varying electric field component in the (t-y) plane. While, beam portions (10 b) and (12 b) also comprise the linearly polarized sinusoidally time-varying forward traveling transverse wave components (18 b) and (24 b), respectively, which are linearly polarized in a plane which is parallel to the given (t-x) plane, and are each associated with a respective linearly polarized sinusoidally time-varying magnetic field component in a respective (t-x) plane.

FIG. (2-a) also illustrates the resultant beam (4 b) aligned along the direction of propagation (26 b) which is parallel to the given (t) axis. Wherein, beam (4 b) is the result of the two combined beam portions (10 b) and (12 b).

Beam portions (10 b) and (12 b) are combined such that wave components (16 b) and (22 b) are superimposed totally out of phase (i.e., 180 degrees out of phase as illustrated according to their alignments with respect to the given y-axis) so as to produce total destructive interference, and the total cancellation of the respectively associated electric field components; and such that wave components (18 b) and (24 b) are superimposed totally out of phase so as to produce total destructive interference, and the total cancellation of the respectively associated magnetic field components. FIG. (2-a) furthermore illustrates the superposition resultant of zero magnitude (28 b) (dashed line) which is associated with the resultant electromagnetic field of zero magnitude in beam (4 b) along the direction of propagation (26 b).

The beam of totally electromagnetically neutralized radiation (4 b) comprises a time-averaged particle flux density of non-zero magnitude, and comprises a time-averaged energy flux density of zero magnitude. Thus, the radiation in beam (4 b) is totally electromagnetically neutralized in direct proportion to (in agreement with) the total elimination of time-averaged energy flux density from beam (4 b) (which includes the total electric charge neutralization of electrically charged particles in a totally electromagnetically neutralized beam in agreement with the corresponding total electromagnetic neutralization of the beam when a beam of totally electromagnetically neutralized electrically charged particles is applied).

FIG. (2-b) illustrates a pulsed beam of totally electromagnetically neutralized radiation (4 c) which is another version of beam (4 a) (illustrated in FIG. 2). Beam (4 c) is a resultant beam which comprises two other combined coherent beam portions of radiation. The beam of totally electromagnetically neutralized radiation (4 c) illustrated in FIG. (2-b) is different from the beam of totally electromagnetically neutralized radiation (4 b) illustrated in FIG. (2-a) in that beam (4 c) is a pulsed beam as illustrated by the three respectively comprised pulses (30 c) and the spaces (32 c) between them.

Pulsed beam (4 c) comprises a time-averaged particle flux density of non-zero magnitude, and comprises a time-averaged energy flux density of zero magnitude. Thus, the radiation in beam (4 c) is totally electromagnetically neutralized.

FIG. (2-c) illustrates an amplitude modulated pulsed beam of totally electromagnetically neutralized radiation (4 d) which is yet another version of beam (4 a) (illustrated in FIG. 2). Beam (4 d) is a resultant beam which comprises still two other combined coherent beam portions of radiation.

The pulsed beam of totally electromagnetically neutralized radiation (4 d) illustrated in FIG. (2-c) is different from the pulsed beam of totally electromagnetically neutralized radiation (4 c) illustrated in FIG. (2-b) in that pulsed beam (4 d) is amplitude modulated so as to digitally encode data (i.e., here, binary digital data 101). Wherein, the (1) digits are each illustrated by one of the two relatively large pulses (30 d) which each comprise a non-zero magnitude of time-averaged particle flux density which is significantly greater than the non-zero magnitude of time-averaged particle flux density of the smaller pulse (30 e), which represents the digit (0), and is situated between the two relatively larger pulses (30 d).

The beam of totally electromagnetically neutralized radiation (4 d) comprises a time-averaged particle flux density of non-zero magnitude, and comprises a time-averaged energy flux density of zero magnitude. Thus, the radiation in beam (4 d) is totally electromagnetically neutralized.

FIG. (3) illustrates a side view of another somewhat more specific preferred embodiment which is applied for transmitting energy in an energy efficient manner. Steps 1) and 2) applied in the preferred embodiment which pertains to FIG. (1) are, in general, applicable in the preferred embodiment illustrated in FIG. (3) except that, more specifically, apparatus (2 f) produces a beam of partly electromagnetically neutralized radiation (4 f) which is coherently transmitted by coherent transmission apparatus (6 f) to target (8 f). In effect, the adverse electromagnetic interaction of neutralized beam (4 f) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 f) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 f) during transmission. Wherein, the adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated. (Note that, conversely, the beam of partly electromagnetically neutralized radiation 4 f can adversely electromagnetically interact with electromagnetically intense entities, e.g., electrically charged particles, comprised in coherent transmission apparatus 6 f in direct proportion to the extent to which the comprised forward traveling transverse waves partly constructively interfere and the associated oscillatorily time-varying electromagnetic fields partly reinforce, i.e., in direct proportion to the time-averaged energy flux density which remains in beam 4 f during transmission. Thus, adverse electromagnetic effects of transmitting energy can be present in this case in direct proportion to the extent to which such adverse electromagnetic interaction is present.)

In the preferred embodiment illustrated in FIG. (3), the beam of partly electromagnetically neutralized radiation (4 f) is coherently transmitted by coherent transmission processes which include: a) potential-energy-based coherent transmission processes which involve a quantum mechanical functional relation between the total energy comprised by the coherently transmitted partly electromagnetically neutralized radiation in beam (4 f) and the potential energy comprised by coherent transmission apparatus (6 f); and b) electromagnetic-based coherent transmission processes which involve electromagnetic interaction between the coherently transmitted partly electromagnetically intense radiation comprised in beam (4 f) and electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 f). (Refer to the preferred embodiment for power transmission which pertains to FIG. 12 a, and the preferred embodiment which applies an optical fiber for wireline communications, for some details of some of the parameters of some example potential-energy-based and electromagnetic-based coherent transmission media.)

FIG. (3-a) illustrates the construction of a beam of partly electromagnetically neutralized radiation (4 h) which is one version of beam (4 f) (illustrated in FIG. 3). The beam of partly electromagnetically neutralized radiation (4 h) illustrated in FIG. (3-a) is different from the beam of totally electromagnetically neutralized radiation (4 b) illustrated in FIG. (2-a) in that beam (4 h) is produced by linearly polarized sinusoidally time-varying electromagnetic wave components which are superimposed only partly out of phase.

Wherein, FIG. (3-a) illustrates intense coherent beam portions of radiation (10 h) and (12 h) which are aligned parallel to the given (t) axis along the directions of propagation (14 h) and (20 h), respectively. Beam portions (10 h) and (12 h) comprise the linearly polarized sinusoidally time-varying forward traveling transverse wave components (16 h) and (22 h), respectively, which are linearly polarized in the (t-y) plane, and are each associated with a respective linearly polarized sinusoidally time-varying electric field component in the (t-y) plane. While, beam portions (10 h) and (12 h) also comprise the linearly polarized sinusoidally time-varying forward traveling transverse wave components (18 h) and (24 h), respectively, which are linearly polarized in a plane which is parallel to the given (t-x) plane, and are each associated with a respective linearly polarized sinusoidally time-varying magnetic field component in a respective (t-x) plane.

FIG. (3-a) furthermore illustrates the resultant beam (4 h) aligned along the direction of propagation (26 h) which is parallel to the given (t) axis. Wherein, beam (4 h) is the result of the two combined beam portions (10 h) and (12 h).

Beam portions (10 h) and (12 h) are combined such that wave components (16 h) and (22 h) are superimposed partly out of phase (i.e., out of phase between zero degrees out of phase and 180 degrees out of phase as illustrated according to their alignments with respect to the given y-axis) so as to produce partial destructive interference, and partial cancellation of the respectively associated electric field components; and such that wave components (18 h) and (24 h) are superimposed partly out of phase (to the same extent as wave components 16 h and 22 h are out of phase) so as to produce partial destructive interference, and partial cancellation of the respectively associated magnetic field components.

The beam of partly electromagnetically neutralized radiation (4 h) comprises a superposition resultant linearly polarized sinusoidally time-varying forward traveling transverse wave (28 h) which comprises the superposition resultant linearly polarized sinusoidally time-varying forward traveling transverse wave component (34 h), which is linearly polarized in the (t-y) plane, and is associated with a resultant linearly polarized sinusoidally time-varying electric field component (in the t-y plane); and wave (28 h) also comprises the superposition resultant linearly polarized sinusoidally time-varying forward traveling transverse wave component (36 h), which is linearly polarized in a plane which is parallel to the (t-x) plane, and is associated with a resultant linearly polarized sinusoidally time-varying magnetic field component in the respective (t-x) plane.

The beam of partly electromagnetically neutralized radiation (4 h) comprises a time-averaged particle flux density of non-zero magnitude, and also comprises a time-averaged energy flux density of non-zero magnitude. In which case, the radiation in beam (4 h) is electromagnetically neutralized in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 h), and is electromagnetically intense in direct proportion to the time-averaged energy flux density which remains in beam (4 h) (wherein partial electromagnetic neutralization of a beam includes the partial electric charge neutralization of electrically charged particles in the electromagnetically neutralized beam in agreement with the corresponding partial electromagnetic neutralization of the beam when a beam of partly electromagnetically neutralized electrically charged particles is applied).

FIG. (3-b) illustrates a pulsed beam of partly electromagnetically neutralized radiation (4 k) which is another version of beam (4 f) (illustrated in FIG. 3). Beam (4 k) is a resultant beam which comprises two other combined coherent beam portions of radiation. The beam of partly electromagnetically neutralized radiation (4 k) illustrated in FIG. (3-b) is different from the beam of partly electromagnetically neutralized radiation (4 h) illustrated in FIG. (3-a) in that beam (4 k) is a pulsed beam as illustrated by the three respectively comprised pulses (30 k) and the spaces (32 k) between them.

Pulsed beam (4 k) comprises a time-averaged particle flux density of non-zero magnitude, and comprises a time-averaged energy flux density of non-zero magnitude. In which case, the radiation in beam (4 k) is electromagnetically neutralized in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 k), and is electromagnetically intense in direct proportion to the time-averaged energy flux density which remains in beam (4 k).

The amplitudes of the superposition resultant waves in the (t-y) plane which are associated with the sinusoidally time-varying electric field components of pulses (30 k) comprised in beam (4 k) would be less than the corresponding amplitudes of the superposition resultant waves which would be associated with the sinusoidally time-varying electric field components of a hypothetical beam of totally electromagnetically intense radiation which would be equivalent to beam (4 k) with the exception that it would be produced with total constructive interference of respectively comprised waves, and total reinforcement of respectively associated electromagnetic fields. Wherein, as a reference, the amplitudes of the superposition resultant waves of pulses (30 k) would be less than the corresponding amplitudes of the superposition resultant waves of the pulses of the hypothetical beam which would be tangent to lines (+y″) and (−y″) illustrated in FIG. (3-b). While, the equivalent would be the case for the amplitudes of the superposition resultant waves which are associated with the sinusoidally time-varying magnetic field components of beam (4 k) in the (t-x) plane as regards to such a hypothetical beam.

FIG. (3-c) illustrates an amplitude modulated pulsed beam of partly electromagnetically neutralized radiation (4 m) which is yet another version of beam (4 f) (illustrated in FIG. 3). Beam (4 m) is a resultant beam which comprises still two other combined coherent beam portions of radiation.

The pulsed beam of partly electromagnetically neutralized radiation (4 m) illustrated in FIG. (3-c) is different from the pulsed beam of partly electromagnetically neutralized radiation (4 k) illustrated in FIG. (3-b) in that pulsed beam (4 m) is amplitude modulated so as to digitally encode data (i.e., here, binary digital data 101). Wherein, the (1) digits are each illustrated by one of the two relatively large pulses (30 m) which each comprise a non-zero magnitude of time-averaged particle flux density which is significantly greater than the time-averaged particle flux density of the smaller pulse (30n), which represents the digit (0), and is situated between the two relatively larger pulses (30 m).

Beam (4 m) comprises a time-averaged particle flux density of non-zero magnitude, and comprises a time-averaged energy flux density of non-zero magnitude. In which case, the radiation in the beam of partly electromagnetically neutralized radiation (4 m) illustrated in FIG. (3-c) is electromagnetically neutralized in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 m), and is electromagnetically intense in direct proportion to the time-averaged energy flux density which remains in beam (4 m).

The amplitudes of the superposition resultant waves of the larger pulses (30 m), and the amplitudes of the superposition resultant wave of the smaller pulse (30n), in the (t-y) plane, which are associated with sinusoidally time-varying electric field components of beam (4 m), would be less than the corresponding amplitudes of the superposition resultant waves which would be associated with the sinusoidally time-varying electric field components of a hypothetical beam of totally electromagnetically intense radiation which would be equivalent to beam (4 m) with the exception that it would be produced with total constructive interference of respectively comprised waves, and total reinforcement of respectively associated electromagnetic fields. Wherein, as references, the amplitudes of the superposition resultant waves of the larger pulses (30 m) would be less than the corresponding amplitudes of the superposition resultant waves of the larger pulses of the hypothetical beam which would be tangent to lines (+y″) and (−y″) illustrated in FIG. (3-c), and the amplitudes of the superposition resultant wave of the smaller pulse (30n) would be less than the corresponding amplitudes of the superposition resultant wave of the smaller pulse of the hypothetical beam which would be tangent to lines (+y′) and (−y′) which are also illustrated in FIG. (3-c). While, the equivalent would be the case for the amplitudes of the superposition resultant waves which are associated with the sinusoidally time-varying magnetic field components of beam (4 m) in the (t-x) plane as regards to such a hypothetical beam.

FIG. (4) illustrates a side view of a generalized preferred embodiment of the present invention which is applied in an effective manner for the transmission and subsequent utilization of a beam of electromagnetically neutralized radiation comprising momentum. Steps 1) and 2) applied in the preferred embodiments which pertain to FIGS. (1), (2), and (3) are, in general, applicable in the preferred embodiment illustrated in FIG. (4) with the addition of a step.

Wherein, in the preferred embodiment illustrated in FIG. (4), apparatus (2 p) produces a beam of electromagnetically neutralized radiation (4 p) comprising a least one significant change in momentum (e.g., at least one transducible change in momentum). In which case, for example, beam (4 p) can comprise a continuous beam of electromagnetically neutralized radiation with a leading edge, or also a trailing edge, as illustrated in the latter case, for example, in FIGS. (2-a) and (3-a); or beam (4 p) can comprise a pulsed beam of electromagnetically neutralized radiation as illustrated, for example, in FIGS. (2-b), (2-c), (3-b), and (3-c). Nevertheless, then, beam (4 p) is coherently transmitted by coherent transmission apparatus (6 p) to targeted momentum-based utilization apparatus (38 p) (e.g., a pressure transducer).

Wherein, the adverse electromagnetic interaction of neutralized beam (4 p) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 p) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 p) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for the respective application (e.g., power attenuation of beam 4 p during transmission) are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

Then, in addition, the preferred embodiment illustrated in FIG. (4) comprises the following step:

Step 3) The utilization of the momentum comprised by the coherently transmitted beam of electromagnetically neutralized radiation (4 p) by utilizing apparatus (38 p). Wherein, coherently transmitted particle beam (4 p) imparts momentum upon apparatus (38 p) which utilizes the applied momentum to produce the result of the respective embodiment, e.g., a targeted pressure transducer can utilize the applied pressure to produce electrical voltage which can then be used for supplying power to a load; or a pressure transducer can utilize the applied pressure to produce electrical voltage comprising retrievable data which can then be used for communications when the momentum comprised by the neutralized particle beam is modulated so as to encode data as, for example, each of the beams of electromagnetically neutralized radiation illustrated in FIGS. (2-c) and (3-c) is modulated so as to encode data. (Note that other than the utilization of voltage, a resulting current can be utilized from, for example, a piezoelectric pressure transducer to produce the result of the respective application of the present invention. Also, note that coherently transmitted particle beam 4 p, which comprises electromagnetically neutralized quanta of electromagnetic radiation or electromagnetically neutralized electrically charged particles, imparts momentum, i.e., applies pressure, upon a pressure transducer in accordance with the law of the conservation of momentum. In which case, momentum, which is comprised by the particles in the neutralized beam, is applied to the pressure transducer by a momentum vector which is equal in magnitude and opposite in direction to the change of the momentum vector of the incident beam of electromagnetically neutralized radiation.)

In other preferred embodiments, the process described in the preferred embodiment which pertains to FIG. (4) is repeated at least once (for the case in which a targeted pressure transducer is applied). Wherein, in each such embodiment, the impinging electromagnetically neutralized particle beam (as described in the preferred embodiment which pertains to FIG. 4) is coherently reflected from the reflective outer surface of a respectively implemented pressure transducer, and then coherently transmitted through coherent transmission apparatus to at least one other pressure transducer and/or back to the first pressure transducer upon which the neutralized particle beam respectively applies pressure which is utilized to produce at least one additional electrical voltage. In which case, upon repetition of the process described in the preferred embodiment which pertains to FIG. (4), but as modified herein, a plurality of electrical voltages are produced during an interval of time to produce the overall net result of the present embodiment, e.g., such that a plurality of electrical voltages are produced for supplying power to a load or loads, or such that data encoded in such electrical voltages are retrieved over an interval of time, e.g., for data buffering or data caching.

FIG. (5) illustrates a side view of another generalized preferred embodiment of the present invention which is applied for the transmission and subsequent utilization of energy in an effective manner. Steps 1) and 2) applied in the preferred embodiment which pertains to FIG. (3) are, in general, applicable in the preferred embodiment illustrated in FIG. (5) with the addition of a step.

In the preferred embodiment illustrated in FIG. (5), apparatus (2 r) produces a beam of partly electromagnetically neutralized radiation (4 r) which is coherently transmitted by coherent transmission apparatus (6 r) to targeted electromagnetic-based utilization apparatus (40 r) (e.g., a photodetector or a particle detector). Wherein, the adverse electromagnetic interaction of the beam of partly electromagnetically neutralized radiation (4 r) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 r) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 r) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for the respective application are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

Then, in addition, the preferred embodiment illustrated in FIG. (5) comprises the following step:

Step 3) The utilization of the coherently transmitted beam of partly electromagnetically neutralized radiation (4 r) by electromagnetic-based utilizing apparatus (40 r) in order to produce the result of the respective embodiment (e.g., a photodetector or a particle detector utilizes transmitted beam 4 r to produce electrical output for photon or electrically charged particle detection when a beam of partly electromagnetically neutralized quanta of electromagnetic radiation or a beam of partly electromagnetically neutralized electrically charged particles is applied, respectively). Wherein, electromagnetically intense entities (e.g., electrically charged particles) comprised in electromagnetic-based utilizing apparatus (40 r) utilize transmitted beam (4 r) by way of electromagnetic interaction.

FIG. (6) illustrates a side view of a generalized conditional preferred embodiment of the present invention which is applied for the transmission and subsequent utilization of energy in an effective manner. In particular, the preferred embodiment illustrated in FIG. (6) is different in that it applies target (8 x) which comprises incoherently scattering and transmitting apparatus (50 x), and a separate posteriorly located electromagnetic-based utilization apparatus (40 x) (e.g., a photodetector or a particle detector). In this case, steps 1) and 2) applied in the preferred embodiments which pertain to FIGS. (1), (2), and (3) are, in general, applicable in the preferred embodiment illustrated in FIG. (6) with the addition of two steps.

Accordingly, in the preferred embodiment illustrated in FIG. (6), apparatus (2 x) produces a beam of electromagnetically neutralized radiation (4 x) which is coherently transmitted by coherent transmission apparatus (6 x) to target (8 x). Wherein, the adverse electromagnetic interaction of neutralized beam (4 x) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 x) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 x) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for the respective application are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

Then, electromagnetically neutralized beam (4 x) is incoherently scattered to an extent by incoherently scattering apparatus in apparatus (50 x) so as to produce a beam of electromagnetically intense radiation (52 x) comprising radiation which comprises randomly distributed transverse waves with random relative phases which neither superimpose nor interfere, such that the electromagnetic field intensities, which are associated with the waves, add, and produce a significant non-zero magnitude of time-averaged energy flux density in apparatus (50 x), i.e., a beam of electromagnetically intense radiation is produced comprising: a) an incoherent beam of radiation produced by incoherent scattering, or also b) any transmitted remaining portion of a beam of partly electromagnetically neutralized radiation which is not incoherently scattered if a beam of partly electromagnetically neutralized radiation is applied. Also in this step, the beam of electromagnetically intense radiation (52 x) is transmitted by transmission apparatus comprised in apparatus (50 x) (e.g., transmission apparatus comprising forward transmitting incoherently scattering media) (or also transmitted by transmission media comprised in electromagnetic-based utilization apparatus 40 x) to electromagnetically intense entities (e.g., electrically charged particles) comprised in apparatus (40 x).

Then, energy is transferred from the transmitted beam of electromagnetically intense radiation (52 x) to utilization apparatus (40 x) in order to produce the result of the respective embodiment (e.g., a photodetector or a particle detector utilizes the transmitted beam of electromagnetically intense radiation 52 x to produce electrical output for photon or electrically charged particle detection when a beam of electromagnetically intense quanta of electromagnetic radiation or a beam of electromagnetically intense electrically charged particles is involved, respectively). Wherein, electromagnetically intense entities (e.g., electrically charged particles) comprised in apparatus (40 x) utilize the transmitted beam of electromagnetically intense radiation by way of electromagnetic interaction.

If a beam of totally electromagnetically neutralized radiation is applied, then the preferred embodiment illustrated in FIG. (6) can apply a step comprising potential-energy-based or also electromagnetic-based incoherent scattering, and, in due course, a step for the utilization of electromagnetically intense radiation. In which case, apparatus (50 x) in the preferred embodiment illustrated in FIG. (6) would comprise potential-energy-based or also electromagnetic-based incoherently scattering apparatus.

However, if a beam of partly electromagnetically neutralized radiation is applied, then the preferred embodiment illustrated in FIG. (6) can apply a step comprising potential-energy-based and/or electromagnetic-based incoherent scattering, and, in due course, a step for the utilization of electromagnetically intense radiation. Wherein, in this case, apparatus (50 x) would comprise potential-energy-based and/or electromagnetic-based incoherently scattering apparatus.

In these cases, potential-energy-based incoherently scattering apparatus can comprise an irregularly ordered distribution of irregularly shaped particles which each comprise: a) a size and spacing which are each comparable to, or significantly larger than, the wavelengths of the waves comprised by the radiation which is incoherently scattered from the beam of electromagnetically neutralized radiation (4 x); and b) potential energy which changes significantly relative to the potential energy of its respective surroundings, and relative to the total energy comprised by the respective incoherently scattered radiation. Wherein, potential-energy-based incoherent scattering processes (e.g., irregular reflections or also irregular refractions) involve a quantum mechanical functional relation between the total energy comprised by the respective incoherently scattered radiation and the potential energy comprised by potential-energy-based incoherently scattering apparatus.

While, electromagnetic-based incoherently scattering apparatus can comprise an irregularly ordered distribution of electromagnetically intense entities (e.g., an irregularly ordered distribution of static particles comprising atoms and/or molecules which comprise electrically charged particles) which each comprise spacing which is significantly larger than the wavelengths of the waves comprised by the respective incoherently scattered electromagnetically intense radiation. In which case, electromagnetic-based incoherent scattering processes involve electromagnetic interaction (e.g., incoherent reradiation scattering when electromagnetically intense quanta of electromagnetic radiation are involved; or incoherent Coulomb-based scattering when electromagnetically intense electrically charged particles are involved).

Note that if a beam of totally electromagnetically neutralized radiation is applied in the preferred embodiment illustrated in FIG. (6), then the onset of electromagnetic-based incoherent scattering of electromagnetically intense radiation by electromagnetic-based incoherently scattering apparatus would occur dependent upon the onset of the production of electromagnetically intense radiation by potential-energy-based incoherent scattering. However, if a beam of partly electromagnetically neutralized radiation is applied in the preferred embodiment illustrated in FIG. (6), then the onset of electromagnetic-based incoherent scattering of electromagnetically intense radiation by electromagnetic-based incoherently scattering apparatus would occur independent of the onset of the production of electromagnetically intense radiation by potential-energy-based incoherent scattering. This would be the case since a beam of partly electromagnetically neutralized radiation is already partly electromagnetically intense due to partial constructive interference of comprised waves and partial reinforcement of respectively associated electromagnetic fields.

Also, note that the time-averaged energy flux density comprised by a given beam of partly electromagnetically neutralized radiation applied in an embodiment facilitates electromagnetic-based incoherent scattering of the given beam of partly electromagnetically neutralized radiation by electromagnetic-based incoherently scattering apparatus in direct proportion to the time-averaged energy flux density comprised in the respectively applied beam of partly electromagnetically neutralized radiation. (Refer to the embodiments which pertain to FIGS. 10 a and 10 b which regard one aspect of the significance of adjusting the time-averaged energy flux density of a beam of electromagnetically neutralized radiation applied in the present invention.)

Furthermore, note that in the method described hereinbefore, the beam of electromagnetically intense radiation produced by incoherent scattering comprises a time-averaged energy flux density which is greater than the time-averaged energy flux density which is comprised by the beam of electromagnetically neutralized radiation from which it is produced. Moreover, note that, in general, in the present invention herein, electromagnetically intense radiation is considered to be radiation which is associated with a non-zero time-averaged energy flux density, such that electromagnetically intense radiation is considered, on average over time, totally electromagnetically intense: a) if it is propagating by itself; b) if it is comprised in a beam of radiation produced with total incoherence; or, in terms of general principles, c) if it is comprised in a coherent beam of totally electromagnetically intense radiation which is produced with total constructive interference of forward traveling transverse waves, and total reinforcement of associated time-varying electromagnetic fields. While, electromagnetically intense radiation is considered, on average over time, partly electromagnetically intense if it is comprised in a coherent beam of partly electromagnetically neutralized radiation which is produced with partial destructive interference of forward traveling transverse waves, and partial cancellation of associated time-varying electromagnetic fields; and produced with partial constructive interference of forward traveling transverse waves, and partial reinforcement of associated time-varying electromagnetic fields.

FIG. (7) illustrates a side view of yet another generalized preferred embodiment of the present invention which is applied for the transmission and subsequent utilization of energy in an effective manner. The steps applied in the preferred embodiment which pertains to FIG. (6) are, in general, applicable in the preferred embodiment illustrated in FIG. (7) except that incoherently scattering and transmitting apparatus is combined with electromagnetic-based utilization apparatus into one apparatus in target apparatus (66 ac) illustrated in FIG. (7) (e.g., a photodetector or a particle detector).

In which case, in the preferred embodiment illustrated in FIG. (7), apparatus (2 ac) produces a beam of electromagnetically neutralized radiation (4 ac) which is coherently transmitted by coherent transmission apparatus (6 ac) to target (66 ac). Wherein, the adverse electromagnetic interaction of neutralized beam (4 ac) with electromagnetically intense entities (e.g., electrically charged particles) comprised in coherent transmission apparatus (6 ac) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 ac) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for the respective application are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

Then, the coherently transmitted electromagnetically neutralized beam (4 ac) is incoherently scattered to an extent by incoherently scattering apparatus comprised in target (66 ac) so as to produce a beam of electromagnetically intense radiation (68 ac) (which comprises a significant non-zero magnitude of time-averaged energy flux density) in target (66 ac), i.e., a beam of electromagnetically intense radiation is produced comprising: a) an incoherent beam of radiation produced by incoherent scattering, or also b) any transmitted remaining portion of a beam of partly electromagnetically neutralized radiation which is not incoherently scattered if a beam of partly electromagnetically neutralized radiation is applied. Also in this step, transmission apparatus comprised in target (66 ac) (e.g., transmission apparatus comprising forward transmitting incoherently scattering media) transmits the beam of electromagnetically intense radiation (68 ac) to electromagnetic-based utilization apparatus (comprising electromagnetically intense entities, e.g., electrically charged particles) also comprised in target (66 ac).

Subsequently, energy is transferred from the transmitted beam of electromagnetically intense radiation (68 ac) to the electromagnetic-based utilization apparatus in target (66 ac) in order to produce the result of the respective embodiment (e.g., a photodetector or a particle detector utilizes the transmitted beam of electromagnetically intense radiation 68 ac to produce electrical output for photon or electrically charged particle detection when a beam of electromagnetically intense quanta of electromagnetic radiation or a beam of electromagnetically intense electrically charged particles is involved, respectively). Wherein, electromagnetically intense entities (e.g., electrically charged particles) comprised in target (66 ac) utilize the transmitted beam of electromagnetically intense radiation by way of electromagnetic interaction. Note that when electromagnetic-based incoherent scattering is applied, then electromagnetic-based incoherent scattering can include electromagnetic-based utilization of electromagnetically intense radiation as, for example, with the application of inelastic incoherent reradiation scattering when a beam of electromagnetically intense quanta of electromagnetic radiation is involved, e.g., with the application of incoherent Compton scattering; or electromagnetic-based incoherent scattering can include electromagnetic-based utilization of electromagnetically intense radiation as, for example, with the application of inelastic incoherent Coulomb-based scattering when a beam of electromagnetically intense electrically charged particles is involved. In which case, a combined incoherent scattering and transmitting step (as with the application of electromagnetic-based forward transmitting incoherently scattering media) can be combined with an electromagnetic-based utilization step.

Still yet another generalized preferred embodiment which is applied for the transmission and subsequent utilization of energy in an effective manner basically applies the steps which are applied in the preferred embodiment which pertains to FIG. (7). However, in this case, some respective modifications are employed including one in which the incoherent scattering apparatus is comprised in the region of the focus of, more specifically, the beam of electromagnetically neutralized electrically charged particles which is applied, and the target itself does not comprise incoherent scattering apparatus which can incoherently scatter a significant amount of radiation from the applied beam of electromagnetically neutralized radiation.

Wherein, in this embodiment, first, apparatus produces a focused pulsed beam of electromagnetically neutralized electrically charged particles (e.g., a focused pulsed beam of electromagnetically neutralized electrons which are electric charge neutralized in direct proportion to the corresponding electromagnetic neutralization of the beam). Then, the neutralized particle beam is coherently transmitted by coherent transmission apparatus to the region of the beam's focus which is positioned in an electromagnetic-based utilization apparatus, which comprises electromagnetically intense entities (e.g., electrically charged particles), and is comprised in a target apparatus. In which case, the adverse electromagnetic interaction of the electromagnetically neutralized particle beam with the coherent transmission apparatus is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the neutralized beam during transmission, such that adverse electromagnetic effects of transmitting energy are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

Then, the focused neutralized particle beam is incoherently scattered to an extent by particles in the region of the beam's focus so as to produce a beam of electromagnetically intense electrically charged particles (comprising a significant non-zero magnitude of time-averaged energy flux density) in the electromagnetic-based utilization apparatus comprised in the target, i.e., a beam of electromagnetically intense electrically charged particles is produced comprising: a) an incoherent beam of electrically charged particles produced by incoherent scattering, or also b) any transmitted remaining portion of a beam of partly electromagnetically neutralized electrically charged particles which is not incoherently scattered if a beam of partly electromagnetically neutralized electrically charged particles is applied.

Here, if a focused beam of totally electromagnetically neutralized electrically charged particles is applied, then incoherently scattering apparatus would initially comprise potential-energy-based incoherently scattering media produced by electrically charged particles in the neutralized particle beam which collectively produce significant incoherently scattering potential energy in the region of the beam's focus. Wherein, the potential-energy-based incoherent scattering media would have parameters equivalent to those parameters of the potential-energy-based incoherently scattering apparatus described in the preferred embodiment which pertains to FIG. (6). However, if a focused beam of partly electromagnetically neutralized electrically charged particles is applied, then the incoherently scattering apparatus can initially comprise electromagnetic-based (i.e., Coulombic-based) incoherently scattering media from electromagnetically intense electrically charged particles in the region of the focus of the partly neutralized particle beam, or also comprise potential-energy-based incoherently scattering media from electrically charged particles in the region of the focus of the partly neutralized particle beam. Wherein, the electromagnetic-based and the potential-energy-based incoherent scattering media would have parameters equivalent to those parameters of the corresponding electromagnetic-based or also potential-energy-based incoherent scattering apparatus described in the preferred embodiment which pertains to FIG. (6).

In either case in which the application of a beam of totally electromagnetically neutralized electrically charged particles is involved, or a beam partly electromagnetically neutralized electrically charged particles is involved, other incoherent scattering apparatus can affect the incoherent scattering outcome of an applied neutralized beam including incoherent scattering apparatus comprising incoherent electromagnetically intense electrically charged particles which are produced as a consequence of the incoherent scattering of the neutralized particle beam in the region of the focus, and/or potential-energy-based and/or electromagnetic-based incoherent scattering media initially present in the target in the region of the beam's focus. Wherein, here also, each such incoherent scattering apparatus would respectively have parameters equivalent to those parameters of the corresponding electromagnetic-based or potential-energy-based incoherently scattering apparatus described in the preferred embodiment which pertains to FIG. (6). While, in addition, such incoherent scattering processes would have the onset conditions for electromagnetic-based incoherent scattering which are also described in the preferred embodiment which pertains to FIG. (6).

Nevertheless, the beam of electromagnetically intense electrically charged particles which is produced by incoherent scattering is then transmitted by the transmission apparatus within the target to electromagnetically intense entities (e.g., electrically charged particles) comprised in the electromagnetic-based utilization apparatus comprised in the target. Then, finally, energy is transferred from the transmitted beam of electromagnetically intense electrically charged particles to the electromagnetic-based utilization apparatus, which then utilizes the transmitted beam of electromagnetically intense electrically charged particles by way of electromagnetic interaction to produce the result of the respective embodiment, e.g., a target comprising a particle detector can utilize the transmitted intense beam to produce electrical output for electrically charged particle detection, or energy can be transferred to a different sort of targeted transducer by, for example, electromagnetic-based absorption or also electromagnetic-based scattering in order to produce a result in the form of, for example, heat motion in, and/or ionization and/or dissociation of, such a target. Note that, in this embodiment also, a combined incoherent scattering and transmitting step (as with the application of electromagnetic-based forward transmitting incoherently scattering media) can be combined with an electromagnetic-based utilization step.

In other preferred embodiments of the present invention, a filtering apparatus is inserted between apparatus which is applied for producing a beam of electromagnetically neutralized radiation and coherent transmission apparatus. Wherein, the filtering apparatus coherently transmits the beam of electromagnetically neutralized radiation while eliminating any unwanted electromagnetically intense radiation which may be produced by systematic and/or random error from the electromagnetically neutralized beam. As examples:

a) A filtering apparatus can comprise coherently transmissive electromagnetically absorptive apparatus for an embodiment of the present invention which applies a beam of electromagnetically neutralized quanta of electromagnetic radiation or a beam of electromagnetically neutralized electrically charged particles, such that any unwanted electromagnetically intense radiation (which may be produced by systematic and/or random error) would be electromagnetically absorbed from a beam of otherwise totally electromagnetically neutralized radiation by such a filtering apparatus. In which case, for example: i) filtering apparatus can comprise coherently transmissive resonance absorptive apparatus for absorbing unwanted relatively long wavelength electromagnetically intense quanta of electromagnetic radiation from a beam of otherwise totally electromagnetically neutralized relatively long wavelength quanta of electromagnetic radiation; ii) filtering apparatus can comprise coherently transmissive edge absorptive apparatus for absorbing unwanted relatively short wavelength electromagnetically intense quanta of electromagnetic radiation from a beam of otherwise totally electromagnetically neutralized short wavelength quanta of electromagnetic radiation, e.g., coherently transmissive k-edge absorptive apparatus for absorbing electromagnetically intense X-rays from a beam of otherwise totally electromagnetically neutralized X-ray wavelength quanta of electromagnetic radiation; or iii) filtering apparatus can comprise apparatus which coherently transmits a beam of electromagnetically neutralized electrically charged particles, and also electromagnetically absorbs unwanted electromagnetically intense electrically charged particles from the otherwise totally electromagnetically neutralized beam;

b) A filtering apparatus can comprise a coherently transmissive limiter apparatus for an embodiment of the present invention which applies a beam of partly electromagnetically neutralized radiation, e.g., an optical limiter for an embodiment which applies a beam of partly electromagnetically neutralized optical wavelength quanta of electromagnetic radiation. Wherein, a beam of partly electromagnetically neutralized radiation which is applied in such an embodiment would be coherently transmitted, and its time-averaged energy flux density would be limited by the limiter filter. In which case, the limiter would eliminate unwanted time-averaged energy flux density (which is produced by systematic and/or random error) from the respectively applied beam of partly electromagnetically neutralized radiation while still coherently transmitting the remaining partly electromagnetically neutralized beam (which still comprises a certain amount of time-averaged energy flux density) towards a target; or

c) A filtering apparatus can comprise a coherently transmissive electrostatic, magnetic, or electromagnetic deflecting apparatus in combination with electromagnetically absorptive apparatus. Wherein, such a filtering apparatus (e.g., comprising a coherently transmissive electrostatic field between two oppositely charged electrostatic plates situated on opposite sides of a neutralized beam) would deflect unwanted electromagnetically intense electrically charged particles (which are produced by systematic and/or random error) out of a beam of otherwise totally electromagnetically neutralized electrically charged particles towards the electromagnetically absorptive apparatus, which would then absorb the unwanted deflected electromagnetically intense electrically charged particles in due course by way of electromagnetic interaction.

In yet other preferred embodiments of the present invention, shielding apparatus is applied to enclose an entire embodiment, or shielding apparatus is applied between only part of a given embodiment and any given material or space in order to shield the environment from electromagnetically neutralized and/or electromagnetically intense radiation which travels beyond a desired boundary around the embodiment of the present invention. For example, a shielding method can comprise steps prior to such a boundary which include: a) the step of incoherently scattering a transgressing beam of radiation, which comprises electromagnetically neutralized radiation, with incoherently scattering apparatus so as to produce a beam of electromagnetically intense radiation comprising a non-zero magnitude of time-averaged energy flux density, i.e., so as to produce a beam of electromagnetically intense radiation comprising: i) an incoherent beam of radiation produced by incoherent scattering, or also ii) any transmitted remaining portion of a beam of partly electromagnetically neutralized radiation which is not incoherently scattered if a beam of partly electromagnetically neutralized radiation is applied; b) the step of transmitting the beam of electromagnetically intense radiation produced as such to an electromagnetic-based absorptive apparatus; and, then, c) the step of absorbing the transmitted electromagnetically intense radiation with the electromagnetic-based absorptive apparatus (which comprises electrically charged particles) by way of electromagnetic interaction. Note that the incoherent scattering step described in step (a) hereinbefore can include the step of transmitting electromagnetically intense radiation to absorptive apparatus which is described in step (b) hereinbefore, such that these steps are combined, e.g., with the application of forward transmitting incoherently scattering media. Also, note that when electromagnetic-based incoherent scattering is applied in step (a) hereinbefore, then electromagnetic-based incoherent scattering can include the electromagnetic-based absorption of electromagnetically intense radiation which is described in step (c) hereinbefore as would be the case with the application of inelastic incoherent reradiation scattering when a beam of electromagnetically intense quanta of electromagnetic radiation is involved, or as would be the case with the application of inelastic incoherent Coulomb-based scattering when a beam of electromagnetically intense electrically charged particles is involved. In which case, a combined incoherent scattering and transmitting step (as with the application of electromagnetic-based forward transmitting incoherently scattering media) can be combined with an electromagnetic-based absorption step, such that steps (a), (b), and (c) hereinbefore can also be combined together.

There are different ways of adjusting the present invention in order to effectively accomplish the result of a respective application including time-averaged particle flux density adjustment, time-averaged energy flux density adjustment, and focal point positioning adjustment. Wherein, one or more ways of adjusting an embodiment of the present invention can be applied in order to effectively accomplish the desired result of an application of the present invention depending on the conditions of the respective application.

FIGS. (8 a) and (8 b) illustrate two embodiments of the present invention which together represent one aspect of the significance of adjusting the time-averaged particle flux density of a beam of electromagnetically neutralized radiation applied in the present invention. In which case, in the embodiments illustrated in FIGS. (8 a) and (8 b), apparatus (2 ak) and (2 am), respectively, produce beams of electromagnetically neutralized radiation (4 ak) and (4 am), respectively. Beams (4 ak) and (4 am) in the two embodiments are equivalent (comprising equivalent radiation with equivalent wavelengths) with the exception that the magnitude of the time-averaged particle flux density in the beam of electromagnetically neutralized radiation (4 ak) illustrated in FIG. (8 a) is less than the time-averaged particle flux density in the beam of electromagnetically neutralized radiation (4 am) illustrated in FIG. (8 b), and with the condition that the time-averaged energy flux density in beam (4 ak) can arbitrarily be the same as, or different from, the time-averaged energy flux density in beam (4 am).

Subsequently, beams (4 ak) and (4 am) are each coherently transmitted by a respectively separate but equivalent coherent transmission apparatus (6 ak) to a respectively separate but equivalent incoherently scattering and transmitting apparatus (50 ak). Wherein, apparatus (50 ak) in the two embodiments are equivalent apparatus which each comprise a uniform distribution of both potential-energy-based and electromagnetic-based incoherently scattering and transmitting apparatus.

Then, beams (4 ak) and (4 am) are each completely scattered in an incoherent manner in its respectively separate but equivalent apparatus (50 ak) so as to produce beams of electromagnetically intense radiation (52 ak) and (52 am), respectively, which each comprise a non-zero magnitude of time-averaged energy flux density. In which case, the beams of electromagnetically intense radiation (52 ak) and (52 am) are each transmitted up to, and through, the centrally located exit plane in its respective incoherently scattering and transmitting apparatus (50 ak), and the time-averaged energy flux density which consequentially fluxes through the respective exit plane in each embodiment is represented by its own distribution curve comprising curves (82) and (84), respectively. Wherein, distribution curves (82) and (84) are each plotted in a (z-y) plane of which the (y) axis is aligned along the centrally located exit plane of the respectively applied apparatus (50 ak) in each embodiment. While, in each of the embodiments illustrated in FIGS. (8 a) and (8 b), a line, comprising line (z″) and line (z″′), respectively, is drawn tangent to the maximum time-averaged energy flux density of the respective distribution curve, and each intersects the respective (z) axis at a point.

In which case, the maximum time-averaged energy flux density which fluxes through the centrally located exit plane in apparatus (50 ak) in the embodiment illustrated in FIG. (8 a) is less than the maximum time-averaged energy flux density which fluxes through the centrally located exit plane in apparatus (50 ak) in the embodiment illustrated in FIG. (8 b) irrespective of whether the time-averaged energy flux density of beam (4 ak) was initially the same as, or different from, the time-averaged energy flux density of beam (4 am). Wherein, such maxima of time-averaged energy flux densities are different as such since the time-averaged particle flux density in the beam of electromagnetically neutralized radiation (4 ak) illustrated in FIG. (8 a) is less than the time-averaged particle flux density in the beam of electromagnetically neutralized radiation (4 am) illustrated in FIG. (8 b), and since apparatus (50 ak) completely incoherently scatters the beam of electromagnetically neutralized radiation applied in each of the embodiments. Thus, the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″) in the embodiment illustrated in FIG. (8 a) is less than the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″′) in the embodiment illustrated in FIG. (8 b). Note that time-averaged particle flux density adjustment can be accomplished herein, for example, by changing the power setting of the source or sources applied to produce a respectively applied beam of electromagnetically neutralized radiation.

FIGS. (9 a) and (9 b) illustrate two embodiments of the present invention which together represent one aspect of the lack of the significance of adjusting the time-averaged energy flux density of a beam of electromagnetically neutralized radiation applied in certain embodiments in the present invention. In which case, in the embodiments illustrated in FIGS. (9 a) and (9 b), apparatus (2 an) and (2 ap), respectively, produce beams of electromagnetically neutralized radiation (4 an) and (4 ap), respectively. Beams (4 an) and (4 ap) each comprise equivalent radiation with equivalent wavelengths, and each comprise an equal magnitude of time-averaged particle flux density, but the two beams are different in that the two forward traveling transverse wave components in each of the two beams are out of phase to relatively different extents such that beams (4 an) and (4 ap) comprise different magnitudes of time-averaged energy flux density.

Subsequently, beams (4 an) and (4 ap) are each coherently transmitted by a respectively separate but equivalent coherent transmission apparatus (6 ak) to a respectively separate but equivalent incoherently scattering and transmitting apparatus (50 ak). Wherein, apparatus (50 ak) in the two embodiments are equivalent apparatus which each comprise a uniform distribution of both potential-energy-based and electromagnetic-based incoherently scattering and transmitting apparatus.

Then, beams (4 an) and (4 ap) are each completely scattered in an incoherent manner in its respectively separate but equivalent apparatus (50 ak) so as to produce beams of electromagnetically intense radiation (52 an) and (52 ap), respectively, which each comprise an equal non-zero magnitude of time-averaged energy flux density. In which case, the beams of electromagnetically intense radiation (52 an) and (52 ap) are each transmitted up to, and through, the centrally located exit plane in its respective incoherently scattering and transmitting apparatus (50 ak), and the time-averaged energy flux density which consequentially fluxes through the respective exit plane in each embodiment is represented by its own distribution curve comprising curves (86) and (88), respectively. Wherein, distribution curves (86) and (88) are each plotted in a (z-y) plane of which the (y) axis is aligned along the centrally located exit plane of the respectively applied apparatus (50 ak) in each embodiment. While, in each of the embodiments illustrated in FIGS. (9 a) and (9 b), a respectively separate but equivalent line (z″) is drawn tangent to the maximum time-averaged energy flux density of the respectively separate but equivalent distribution curve, and each intersects the respective (z) axis at a point.

In which case, the maximum time-averaged energy flux density which fluxes through the centrally located exit plane in apparatus (50 ak) in the embodiment illustrated in FIG. (9 a) is equal to the maximum time-averaged energy flux density which fluxes through the centrally located exit plane in apparatus (50 ak) in the embodiment illustrated in FIG. (9 b) irrespective of the difference in the magnitude of the time-averaged energy flux density of beam (4 an) compared to the time-averaged energy flux density of beam (4 ap). Wherein, such maxima of time-averaged energy flux densities are the same as such since the time-averaged particle flux density in the beam of electromagnetically neutralized radiation (4 an) in the embodiment illustrated in FIG. (9 a) is equal to the time-averaged particle flux density in the beam of electromagnetically neutralized radiation (4 ap) in the embodiment illustrated in FIG. (9 b), and since apparatus (50 ak) in each of the embodiments completely incoherently scatters the beam of electromagnetically neutralized radiation which is respectively applied. Thus, the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″) in the embodiment illustrated in FIG. (9 a) is equal to the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″) in the embodiment illustrated in FIG. (9 b). (Note that time-averaged energy flux density adjustment can be accomplished by changing the relative phases of the waves, i.e., here, by changing the relative phase of the transverse wave components, which are comprised in a respectively applied beam of electromagnetically neutralized radiation.)

FIGS. (10 a) and (10 b) illustrate two embodiments of the present invention which together represent one aspect of the significance of adjusting the time-averaged energy flux density of a beam of electromagnetically neutralized radiation applied in the present invention. In which case, in the embodiments illustrated in FIGS. (10 a) and (10 b), apparatus (2 ar) and (2 at), respectively, produce beams of electromagnetically neutralized radiation (4 ar) and (4 at), respectively. Beams (4 ar) and (4 at) each comprise equivalent radiation with equivalent wavelengths, and each comprise an equal magnitude of time-averaged particle flux density, but the two beams are different in that beam (4 ar) comprises forward traveling transverse wave components which are out of phase to a greater extent than the forward traveling transverse wave components of beam (4 at), such that the beam of electromagnetically neutralized radiation (4 ar) comprises less time-averaged energy flux density than the beam of electromagnetically neutralized radiation (4 at).

Subsequently, beams (4 ar) and (4 at) are each coherently transmitted by a respectively separate but equivalent coherent transmission apparatus (6 ak) to a respectively separate but equivalent incoherently scattering and transmitting apparatus (50 ar). Wherein, apparatus (50 ar) in the two embodiments are equivalent apparatus which each comprise a uniform distribution of both potential-energy-based and electromagnetic-based incoherently scattering and transmitting apparatus.

Then, beams (4 ar) and (4 at) are each partially scattered in an incoherent manner in its respectively separate but equivalent apparatus (50 ar) so as to produce beams of electromagnetically intense radiation (52 ar) and (52 at), respectively, which each comprise a non-zero magnitude of time-averaged energy flux density. In which case, the beams of electromagnetically intense radiation (52 ar) and (52 at) are each transmitted up to, and through, the centrally located exit plane in its respective incoherently scattering and transmitting apparatus (50 ar), and the time-averaged energy flux density which consequentially fluxes through the respective exit plane in each embodiment is represented by its own distribution curve comprising curves (90) and (92), respectively. Wherein, distribution curves (90) and (92) are each plotted in a (z-y) plane of which the (y) axis is aligned along the centrally located exit plane of the respectively applied apparatus (50 ar) in each embodiment. While, in each of the embodiments illustrated in FIGS. (10 a) and (10 b), a line, comprising line (z′) and line (z″), respectively, is drawn tangent to the maximum time-averaged energy flux density of the respective distribution curve, and each intersects the respective (z) axis at a point.

Here, even though the time-averaged particle flux densities of electromagnetically neutralized beams (4 ar) and (4 at) in the embodiments illustrated in FIGS. (10 a) and (10 b) are equal, the incoherently scattering apparatus in apparatus (50 ar) in each of the embodiments only partially incoherently scatters the respectively applied beam of electromagnetically neutralized radiation such that electromagnetic-based incoherently scattering has a greater effect in apparatus (50 ar) in the embodiment illustrated in FIG. (10 b), since the beam of electromagnetically neutralized radiation (4 at), in the embodiment illustrated in FIG. (10 b), comprises a greater time-averaged energy flux density than the beam of electromagnetically neutralized radiation (4 ar) in the embodiment illustrated in FIG. (10 a). Wherein, the time-averaged energy flux density in beam (4 at) facilitates electromagnetic-based incoherent scattering in apparatus (50 ar) in the embodiment illustrated in FIG. (10 b) to a greater extent than time-averaged energy flux density in beam (4 ar) facilitates electromagnetic-based incoherently scattering in apparatus (50 ar) in the embodiment illustrated in FIG. (10 a).

Thus, the maximum time-averaged energy flux density which fluxes through the centrally located exit plane in apparatus (50 ar) in the embodiment illustrated in FIG. (10 a) is less than the maximum time-averaged energy flux density which fluxes through the centrally located exit plane in apparatus (50 ar) in the embodiment illustrated in FIG. (10 b). Therefore, the distance on the (z) axis between (0) (zero) and the intersecting point of line (z′) in the embodiment illustrated in FIG. (10 a) is less than the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″) in the embodiment illustrated in FIG. (10 b).

FIGS. (11 a) and (11 b) illustrate two embodiments of the present invention which together represent one aspect of the significance of adjusting the depth of the focal point of an applied beam of electromagnetically neutralized radiation in the target of the present invention. In which case, in each of the two embodiments illustrated in FIGS. (11 a) and (11 b), a respectively separate but equivalent apparatus (2au) produces a respectively separate but equivalent focused beam of electromagnetically neutralized radiation (4 au), which both comprise equivalent radiation with equivalent wavelengths, both comprise an equal magnitude of time-averaged particle flux density, and both comprise an equal magnitude of time-averaged energy flux density, but the two beams are different in that each beam is focused towards a focal point which is positioned at a different depth in a respectively separate but equivalent incoherently scattering and transmitting apparatus (50 ak).

Subsequently, the beams of electromagnetically neutralized radiation (4 au) in the two embodiments illustrated in FIGS. (11 a) and (11 b) are each coherently transmitted by a respectively separate but equivalent (except for their lengths) coherent transmission apparatus (6 ak) to a respectively separate but equivalent incoherently scattering and transmitting apparatus (50 ak). Wherein, apparatus (50 ak) in the two embodiments are equivalent apparatus which each comprise a uniform distribution of both potential-energy-based and electromagnetic-based incoherently scattering and transmitting apparatus.

Then, in the two embodiments illustrated in FIGS. (11 a) and (11 b), the respectively separate but equivalent coherently transmitted beams of electromagnetically neutralized radiation (4 au) are each incoherently scattered to a respective extent by its respectively separate but equivalent apparatus (50 ak) so as to produce beams of electromagnetically intense radiation (52 au) and (52 av), respectively, which each comprise a respective non-zero magnitude of time-averaged energy flux density. In which case, the beams of electromagnetically intense radiation (52 au) and (52 av) are each transmitted up to, and through, the focal plane at a respective depth within its respective incoherently scattering and transmitting apparatus (50 ak), and the time-averaged energy flux density which consequentially fluxes through the focal plane in each embodiment is represented by its own distribution curve comprising curves (94) and (96), respectively. Wherein, distribution curves (94) and (96) are each plotted in a (z-y) plane of which the (y) axis is aligned along the focal plane of the applied beam in the respectively applied apparatus (50 ak) in each embodiment. While, in each of the embodiments illustrated in FIGS. (11 a) and (11 b), a line, comprising line (z″) and line (z″′), respectively, is drawn tangent to the maximum time-averaged energy flux density of the respective distribution curve, and each intersects the respective (z) axis at a point.

Here, the focal point of beam (4 au) is positioned in the incoherently scattering and transmitting apparatus (50 ak) in the embodiment illustrated in FIG. (11 a) at a lesser depth than the depth at which the focal point of beam (4 au) is positioned in the incoherently scattering and transmitting apparatus (50 ak) in the embodiment illustrated in FIG. (11 b). Wherein, the number of incoherent scatterers in the path of the beam of electromagnetically neutralized radiation (4 au) anterior to the focus in the embodiment illustrated in FIG. (11 a) is less than the number of incoherent scatterers in the path of the beam of electromagnetically neutralized radiation (4 au) anterior to the focus in the embodiment illustrated in FIG. (11 b).

In which case, incoherently scattering apparatus in apparatus (50 ak) in the embodiment illustrated in FIG. (11 a) incoherently scatters the respectively applied beam of electromagnetically neutralized radiation (4 au) to a lesser extent anterior to its focal point than incoherently scattering apparatus in apparatus (50ak) incoherently scatters the respectively applied beam of electromagnetically neutralized radiation (4 au) anterior to its focal point in the embodiment illustrated in FIG. (11 b). Thus, the maximum time-averaged energy flux density which fluxes through the focal plane in apparatus (50 ak) in the embodiment illustrated in FIG. (11 a) is less than the maximum time-averaged energy flux density which fluxes through the focal plane in apparatus (50 ak) in the embodiment illustrated in FIG. (11 b). Therefore, the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″) in the embodiment in FIG. (11 a) is less than the distance on the (z) axis between (0) (zero) and the intersecting point of line (z″′) in the embodiment illustrated in FIG. (11 b).

FIG. (12 a) is an illustration of a side view of a somewhat specific preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and includes a longitudinally sectioned view of the respectively applied air filled tubing. The steps applied in preferred embodiments which pertain to FIGS. (4), (5), (6), and (7) are, in general, applicable in the preferred embodiment illustrated in FIG. (12 a) with some respective modifications.

In the preferred embodiment illustrated in FIG. (12 a), apparatus (2 cf), which comprises a source of electromagnetically intense coherent forward propagating radiation and interferometric apparatus (e.g., apparatus which is equivalent to the version of Michelson interferometric apparatus illustrated in FIG. 1′), produces a beam of electromagnetically neutralized radiation (4 cf) which is coherently transmitted by coherent transmission media comprising air (6 cf) and tubing (or hollow cylindrical guide) (6 ch) to power utilization apparatus (8 cf). Wherein, the adverse electromagnetic interaction of neutralized beam (4 cf) with electrically charged particles comprised in air (6 cf) and tubing (6 ch) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 cf) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for power are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated (e.g., power attenuation of beam 4 cf is eliminated to an extent such that energy is conserved during transmission, and, consequentially, the inefficiency of transmitting energy is eliminated to a corresponding extent).

In this case, a) coherently transmitting tubing (6 ch) comprises tubing walls which produce a potential energy barrier which: i) changes significantly relative to the potential energy comprised by its respective surroundings (i.e., here, air 6 cf inside, and air outside, tubing 6 ch), and ii) changes significantly relative to the total energy comprised by the coherently transmitted electromagnetically neutralized radiation in beam (4 cf); and b) coherently transmitting tubing (6 ch) comprises particles, which comprise electrically charged particles, on the inner surface which each comprise a size and spacing which are each significantly smaller than the wavelengths of the waves comprised by the coherently transmitted radiation in beam (4 cf). Wherein, coherent transmission processes involve a quantum mechanical functional relation between the total energy comprised by the coherently transmitted electromagnetically neutralized radiation in beam (4 cf) and the potential energy comprised by tubing (6 ch).

However, more specifically, if a beam of partly electromagnetically neutralized radiation, which comprises, for example, a very small time-averaged energy flux density, is applied, then coherent transmission processes also involve electromagnetic interaction between coherently transmitted electromagnetically intense radiation in beam (4 cf) and electrically charged particles comprised in air (6 cf) and tubing (6 ch). In which case, electromagnetic-based coherent transmission media would comprise electrically charged particles on the inner surface of tubing (6 ch) which each comprise a size and spacing which are each significantly smaller than the wavelengths of the waves comprised by the coherently transmitted beam of partly electromagnetically neutralized radiation. Wherein, if a beam of partly electromagnetically neutralized radiation is applied, then the tubing walls should also be as electromagnetically non-absorptive as possible.

Nevertheless, then, energy is transferred from the transmitted beam to power utilization apparatus (8 cf) in order to produce the result of the respective embodiment by a power utilization process which comprises one of the following examples depending upon the embodiment applied: a) a power utilization process in which a momentum-based utilization apparatus utilizes the momentum applied by a transmitted beam of electromagnetically neutralized radiation, e.g., a pressure transducer utilizes the pressure applied by a transmitted electromagnetically neutralized particle beam (comprising electromagnetically neutralized quanta of electromagnetic radiation or electromagnetically neutralized electrically charged particles) in order to produce electrical voltage for supplying power to a load or loads (as described generally in the preferred embodiment which pertains to FIG. 4); b) a power utilization process in which electromagnetic-based utilization apparatus, which comprises electrically charged particles, utilizes a transmitted beam of partly electromagnetically neutralized radiation by way of electromagnetic interaction when a beam of partly electromagnetically neutralized radiation is applied (as described generally in the preferred embodiment which pertains to FIG. 5), e.g., a photodetector or a particle detector utilizes a transmitted beam of partly electromagnetically neutralized radiation in order to produce electrical output for supplying power to a load; or c) a power utilization process which includes: i) the step of incoherently scattering a transmitted beam of electromagnetically neutralized radiation with incoherently scattering media so as to produce a beam of electromagnetically intense radiation comprising a significant non-zero magnitude of time-averaged energy flux density, i.e., so as to produce a beam of electromagnetically intense radiation comprising an incoherent beam of radiation which is produced by incoherent scattering, or also comprising any transmitted remaining portion of a beam of partly electromagnetically neutralized radiation which is not incoherently scattered if a beam of partly electromagnetically neutralized radiation is applied; ii) the step of transmitting the beam of electromagnetically intense radiation produced as such with transmission media to an electromagnetic-based utilization apparatus; and then iii) the step of utilizing the transmitted beam of electromagnetically intense radiation with electromagnetic-based utilization apparatus comprising electrically charged particles (by way of electromagnetic interaction) for power (as described generally in, for example, the preferred embodiment which pertains to FIG. 6), e.g., a photodetector or a particle detector utilizes a transmitted beam of electromagnetically intense radiation in order to produce electrical output for supplying power to a load.

Note that the incoherent scattering step which is described in step (i) hereinbefore can include the step of transmitting the electromagnetically intense radiation to the utilization apparatus which is described in step (ii) hereinbefore, such that these steps are combined (e.g., as with the application of forward transmitting incoherently scattering media). Also, note that when electromagnetic-based incoherent scattering is applied in step (i) hereinbefore, then electromagnetic-based incoherent scattering can include the electromagnetic-based utilization of electromagnetically intense radiation which is described in step (iii) hereinbefore as would be the case with the application of inelastic incoherent reradiation scattering when a beam of electromagnetically intense quanta of electromagnetic radiation is involved, or as would be the case with the application of inelastic incoherent Coulomb-based scattering when a beam of electromagnetically intense electrically charged particles is involved. In which case, a combined incoherent scattering and transmitting step (as with the application of electromagnetic-based forward transmitting incoherently scattering media) can be combined with an electromagnetic-based utilization step, such that steps (i), (ii), and (iii) hereinbefore can be combined together.

Furthermore, note that this preferred embodiment of the present invention can be applied for achieving a form of electromagnetically “resistance-less” power transmission when a beam of totally electromagnetically neutralized radiation is applied, or a form of electromagnetically “low-resistance” power transmission when a beam of partly electromagnetically neutralized radiation is applied. Moreover, note that if a beam of electromagnetically neutralized electrons is transmitted to a targeted utilization apparatus, and the transmitted electromagnetically neutralized electrons subsequently become static in the utilization apparatus by, for example, scattering, then the electromagnetically neutralized electrons will become electromagnetically intense electrons upon becoming static, and can then be utilized to produce an electrical voltage, i.e., a potential energy gradient.

FIG. (12 b) is an illustration of a side view of a somewhat different preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and also includes a longitudinally sectioned view of the respectively applied air filled tubing. The steps applied in the preferred embodiment illustrated in FIG. (12 a) are applicable in the preferred embodiment illustrated in FIG. (12 b) except that, as a modification, two tube sections merge into a single section of tubing (i.e., the merged tubing acts as a coupler).

Wherein, in the preferred embodiment illustrated in FIG. (12 b), apparatus (2 ck) and (2 cm) produce beams of electromagnetically neutralized radiation (4 ck) and (4 cm), respectively, which are coherently transmitted by tube sections (6 ck) and (6 cm), respectively, to a merged section of tubing (6 cn). Then, neutralized beams (4 ck) and (4 cm) are combined by the merged section of tubing (6 cn) into a single beam of electromagnetically neutralized radiation (4 cn) which is transmitted in a coherent manner by the merged section of tubing (6 cn) to, and utilized in due course by, power utilization apparatus (8 ck).

FIG. (12 c) is an illustration of a side view of another somewhat different preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and also includes a longitudinally sectioned view of the respectively applied air filled tubing. The steps applied in the preferred embodiment illustrated in FIG. (12 a) are applicable in the preferred embodiment illustrated in FIG. (12 c) except that, as a modification, the applied tubing branches into two sections of tubing (i.e., the branched tubing acts as a splitter).

Wherein, in the preferred embodiment illustrated in FIG. (12 c), apparatus (2 cp) produces a beam of electromagnetically neutralized radiation (4 cp) which is coherently transmitted by tube section (6 cp) to a branched section of tubing, and then is divided by the branched section of tubing into beam fractions of electromagnetically neutralized radiation (4 cr) and (4 ct). Then, tube sections (6 cr) and (6 ct) transmit neutralized beam fractions (4 cr) and (4 ct), respectively, in a coherent manner to power utilization apparatus (8 cr) and (8 ct), respectively, which then each utilize the respectively transmitted neutralized beam fraction for power in due course.

FIG. (12 d) is an illustration of a side view of yet another somewhat different preferred embodiment of the present invention which is applied for transmitting power in an effective manner, and also includes a longitudinally sectioned view of the respectively applied air filled tubing. The steps applied in the preferred embodiments illustrated in FIGS. (12 a), (12 b), and (12 c) are applicable in the preferred embodiment illustrated in FIG. (12 d) except that, as a modification, two sections of tubing merge into a single section of tubing (i.e., the merged tubing acts as a coupler), and then the single section of tubing branches into two sections of tubing (i.e., the branched tubing acts as a splitter).

Wherein, in the preferred embodiment illustrated in FIG. (12 d), apparatus (2 cu) and (2 cv) produce beams of electromagnetically neutralized radiation (4 cu) and (4 cv), respectively, which are coherently transmitted by tube sections (6 cu) and (6 cv), respectively, to a merged section of tubing (6 cw). Then, neutralized beam fractions (4 cu) and (4 cv) are combined by the merged section of tubing (6 cw) into a single beam of electromagnetically neutralized radiation (4 cw) which is coherently transmitted by the merged section of tubing (6 cw) to a branched section of tubing which then divides beam (4 cw) into beam fractions of electromagnetically neutralized radiation (4 cx) and (4 cy). Subsequently, neutralized beam fractions (4 cx) and (4 cy) are coherently transmitted by tube sections (6 cx) and (6 cy), respectively, to power utilization apparatus (8 cx) and (8 cy), respectively, which then each utilize the respectively transmitted neutralized beam fraction for power in due course.

FIG. (13) is an illustration of a side view of a somewhat specific preferred embodiment of the present invention which is applied for transmitting data in an effective manner for wireline communications, and includes a longitudinally sectioned view of the air filled tubing which is respectively applied for data transmission. The steps applied in the preferred embodiments for power transmission which pertain to FIGS. (12 a), (12 b), (12 c), and (12 d) are, in general, applicable in the preferred embodiment for wireline communications herein with some respective modifications.

In which case, in the preferred embodiment illustrated in FIG. (13), apparatus (2 da) comprises transmitter apparatus (2 db) which comprises a miniature laser source and interferometric apparatus. Wherein, apparatus (2 db) produces a beam of electromagnetically neutralized quanta of electromagnetic radiation (4 da ₁).

Then, beam (4 da ₁) is coherently transmitted by coherent transmission media comprising air to modulator (98 da), and then coherently transmitted and modulated by modulator (98 da), which comprises coherent transmission media, and changes its respective potential energy in order to modulate (e.g., a coherently transmissive acousto-optic modulator) so as to produce a modulated beam of electromagnetically neutralized quanta of electromagnetic radiation (4 da ₂) (e.g., an amplitude modulated beam of electromagnetically neutralized quanta of electromagnetic radiation which digitally encodes data in a manner which is substantially equivalent to the manner in which each of the beams of electromagnetically neutralized radiation illustrated in FIGS. 2-c and 3-c digitally encodes data). Nevertheless, then, beam (4 da ₂) is coherently transmitted by air comprised in apparatus (2 da) so as to exit apparatus (2 da).

Then, the modulated beam of electromagnetically neutralized quanta of electromagnetic radiation (4 da ₂) is coherently transmitted by coherent transmission media comprising air (6 da) and tubing (or hollow cylindrical guide) (6 db) of single mode dimensions to receiver apparatus (8 da). Wherein, the adverse electromagnetic interaction of neutralized beam (4 da ₂) with electrically charged particles comprised in air (6 da) and tubing (6 db) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 da ₂) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for wireline communications are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated. As examples, with respect to a prior art fiber optic system: a) The present invention eliminates signal attenuation in direct proportion to the time-averaged energy flux density which is eliminated from the electromagnetically neutralized beam during transmission so as to increase the distance a signal can travel at various wavelengths without being amplified (or repeated), such that the need for relatively high transmitter power output and/or the need for signal amplification (or repeating) is eliminated to a directly proportional extent, and such that the bandwidth available for wireline communications (in terms of frequencies) is increased; b) The present invention decreases the refractive index of the transmitting medium relative to an optical fiber, such that the speed at which a signal travels is increased to a directly proportional extent, and thus the bandwidth available for wireline communications is correspondingly increased in this way (i.e., in terms of the speed of data transmission); and c) The present invention eliminates some of the complexities of making and deploying a conveying medium for high bandwidth data transmission for wireline communications by applying air filled tubing instead of optical fiber.

Then, beam (4 da ₂) is utilized by an appropriate process for communications reception by receiving apparatus (8 da). Wherein, beam (4 da ₂) is utilized, for example, by one of the power utilizing processes which are described in the preferred embodiment which pertains to FIG. (12 a) except that the data encoded in the power of the coherently transmitted modulated beam of electromagnetically neutralized quanta of electromagnetic radiation (4 da ₂) is utilized by receiving apparatus (8 da) for communications.

FIG. (14) illustrates a side view of another somewhat specific preferred embodiment of the present invention which is applied for transmitting data for wireline communications in an effective manner. The steps applied in the preferred embodiment which pertains to FIG. (13) are, in general, applicable in the preferred embodiment illustrated in FIG. (14) with some respective modifications for the method of communications employed herein which applies wave division multiplexing and demultiplexing.

Wherein, in the preferred embodiment illustrated in FIG. (14), apparatus (2 dc) comprises a plurality of transmitter apparatus (2 dd), (2 de), and (2 df) which each comprise a miniature laser source (which each produce a laser beam comprising an exclusive linewidth), and interferometric apparatus. In which case, apparatus (2 dd), (2 de), and (2 df) each produce a beam of electromagnetically neutralized quanta of electromagnetic radiation comprising beams (4 dd ₁), (4 de ₁), and (4 df ₁), respectively. Then, beams (4 dd ₁), (4 de ₁), and (4 df ₁), which comprise respectively different linewidths, are coherently transmitted by coherent transmission media comprising air to modulators (98 dd), (98 de), and (98 df), respectively. Beams (4 dd ₁), (4 de ₁), and (4 df ₁) are then modulated and coherently transmitted by modulators (98 dd), (98 de), and (98 df), respectively (which each modulate by changing its respective potential energy, e.g., each comprises a coherently transmissive acousto-optic modulator), so as to produce modulated beams of electromagnetically neutralized quanta of electromagnetic radiation (4 dd ₂), (4 de ₂), and (4 df ₂), respectively, which each encodes data (e.g., an amplitude modulated beam of electromagnetically neutralized quanta of electromagnetic radiation which digitally encodes data in a manner which is substantially equivalent to the manner in which each of the beams of electromagnetically neutralized radiation illustrated in FIGS. 2-c and 3-c digitally encodes data). Subsequently, beams (4 dd ₂), (4 de ₂), and (4 df ₂) are coherently transmitted by air to, and multiplexed by, multiplexer (100 dc) so as to produce a multiplexed beam of electromagnetically neutralized quanta of electromagnetic radiation (4 dc).

After that, the neutralized multiplexed beam (4 dc) is coherently transmitted by coherent transmission media comprising air (6 dc) and tubing (6 dd) of single mode dimensions to demultiplexer (102 dc). Wherein, the adverse electromagnetic interaction of multiplexed beam (4 dc) with electrically charged particles comprised in air (6 dc) and tubing (6 dd) is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from beam (4 dc) during transmission. In which case, the adverse electromagnetic effects of transmitting energy for wireline communications are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated (which includes the elimination of the example adverse electromagnetic effects which are eliminated in the preferred embodiment which pertains to FIG. 13).

Next, demultiplexer (102 dc) demultiplexes beam (4 dc) into separate modulated beams of electromagnetically neutralized quanta of electromagnetic radiation of respective linewidths comprising beams (4 dd ₃), (4 de ₃), and (4 df ₃), which are then coherently transmitted to receiver apparatus (8 dd), (8 de), and (8 df), respectively, which are collectively comprised in receiver apparatus (8 dc). Wherein, the utilization apparatus comprised in each of the receiver apparatus (8 dd), (8 de), and (8 df) then utilizes the respectively transmitted modulated neutralized beam by an appropriate process for communications reception (e.g., one of the receiving processes described in the preferred embodiment which pertains to FIG. 13, i.e., for example, by one of the power utilizing processes which are described in the preferred embodiment which pertains to FIG. 12 a except that the data encoded in the power of each modulated beam of electromagnetically neutralized quanta of electromagnetic radiation herein is utilized by a respective receiving apparatus for communications).

FIG. (14′) is a somewhat detailed illustration of one version of the preferred embodiment of the present invention illustrated in FIG. (14). In which case, FIG. (14′) especially illustrates multiplexer (100 dc′-A) which is one version of multiplexer (100 dc) illustrated in FIG. (14), and also especially illustrates demultiplexer (102 dc′-A) which is one version of demultiplexer (102dc) illustrated in FIG. (14). Wherein, the steps applied in the preferred embodiment which pertains to FIG. (14), which comprises a method which applies multiplexing and demultiplexing for transmitting data in an effective manner for wireline communications, are, in general, applicable in the preferred embodiment illustrated in FIG. (14′) except that, more specifically, the preferred embodiment illustrated in FIG. (14′) applies multiplexer (100 dc′-A) which comprises prism (100 dc′-B), and applies demultiplexer (102 dc′-A) which comprises prism (102 dc′-B).

Other preferred embodiments for transmitting data in an effective manner for wireline communications apply methods which are generally equivalent to, but somewhat more specifically different from, the methods applied in the preferred embodiments which pertain to FIGS. (13) and (14) which are exemplified by the application of electromagnetically neutralized optical wavelengths of quanta of electromagnetic radiation. Wherein, these preferred embodiments herein are somewhat different in that they are respectively modified for the specific application of tubing of single mode dimensions with the inclusive transmission of longer wavelengths of quanta of electromagnetic radiation relative to the optical wavelengths.

Still other preferred embodiments for transmitting data in an effective manner for wireline communications are different in that each applies a method which applies optical fiber as a coherent transmission medium instead of air filled tubing as applied in the preferred embodiments which pertain to FIGS. (13), (14), and (14′). Wherein, in one such preferred embodiment, apparatus, which comprises a miniature laser and interferometric apparatus, produces a data encoded modulated beam of electromagnetically neutralized quanta of electromagnetic radiation (e.g., an amplitude modulated beam of electromagnetically neutralized quanta of electromagnetic radiation which digitally encodes data in a manner which is substantially equivalent to the manner in which each of the beams of electromagnetically neutralized radiation illustrated in FIGS. 2-c and 3-c digitally encodes data). Then, the neutralized beam is coherently transmitted by an optical fiber to a receiver apparatus.

In which case, the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the optical fiber is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the coherently transmitted neutralized beam during transmission. Wherein, the adverse electromagnetic effects of transmitting energy for wireline communications (e.g., signal attenuation) are eliminated in direct proportion to the extent to which such adverse electromagnetic interaction is eliminated.

The coherently transmitting optical fiber comprises an optical fiber core which comprises potential energy which changes significantly relative to the potential energy comprised by the respectively comprised cladding, and relative to the total energy comprised by the coherently transmitted electromagnetically neutralized quanta of electromagnetic radiation so as to produce a significant potential energy barrier (which effectively produces total internal reflection). While, the optical fiber core also comprises particles, comprising electrically charged particles, which each comprise: a) a size and spacing which are each significantly smaller than the wavelengths of the waves of the quanta of electromagnetic radiation comprised in the coherently transmitted neutralized beam; and b) potential energy which changes insignificantly relative to the potential energy comprised by its respective surroundings, and relative to the total energy comprised by the electromagnetically neutralized quanta of electromagnetic radiation which are coherently transmitted inside the optical fiber core. Wherein, coherent transmission processes involve a quantum mechanical functional relation between the total energy comprised by the coherently transmitted electromagnetically neutralized quanta of electromagnetic radiation and the potential energy comprised by the optical fiber; or, also, coherent transmission processes involve electromagnetic interaction between electromagnetically intense quanta of electromagnetic radiation in the neutralized beam and electrically charged particles comprised in the optical fiber if a modulated beam of partly electromagnetically neutralized quanta of electromagnetic radiation is applied. In which case, electromagnetic-based coherent transmission media would comprise electrically charged particles in the optical fiber core which each comprise a size and spacing which are each significantly smaller than the wavelengths of the waves comprised by the coherently transmitted beam of partly electromagnetically neutralized radiation.

Then, receiver apparatus utilizes the transmitted neutralized beam by an appropriate process for communications reception. Wherein, for example, receiving apparatus utilizes the transmitted beam by one of the power utilizing processes which are described in the preferred embodiment which pertains to FIG. (12 a) except that the data encoded in the power of the modulated neutralized beam is utilized by receiving apparatus for communications.

Still yet other preferred embodiments of the present invention each employ a method which is both applied for transmitting power for use as a utility as described in the preferred embodiments which pertain to FIGS. (12 a), (12 b), (12 c), and (12 d); and also applied for transmitting power in the form of data for communications as described in the preferred embodiments which pertain to FIGS. (13), (14), and (14′), the preferred embodiments which specifically include the application of relatively long wavelengths of electromagnetically neutralized quanta of electromagnetic radiation relative to optical wavelengths (which are referred to immediately following the embodiment which pertains to FIG. (14′), and the preferred embodiments which apply optical fiber (described above). In which case, in each such embodiment, the target utilizes the power of the transmitted modulated beam of electromagnetically neutralized radiation for power per se by, for example, one of the power utilizing processes which are described in the preferred embodiment which pertains to FIG. (12 a), and also utilizes the data encoded in the same transmitted beam for communications by one of the receiving processes described in the preferred embodiment which pertains to FIG. (13), i.e., for example, one of the power utilizing processes which are described in the preferred embodiment which pertains to FIG. (12 a) except that the data encoded in the power of the transmitted neutralized beam is utilized by receiving apparatus for communications.

FIGS. (15) and (16) each illustrate a side view of a somewhat specific preferred embodiment of the present invention which is applied for transmitting data in an effective manner for wireless communications. The steps applied in the preferred embodiment which pertains to FIG. (13) for wireline communications, and the preferred embodiments for wireline communications which specifically include the application of relatively long wavelengths of electromagnetically neutralized quanta of electromagnetic radiation relative to optical wavelengths (which are referred to immediately following the preferred embodiment pertaining to FIG. 14′, and which are applicable to the preferred embodiment which pertains to FIG. (13), are, in general, applicable in the preferred embodiment for wireless communications illustrated in FIG. (15) with respective modifications including the application of only air (6 dh) as a coherent transmission medium instead of air filled tubing. While, the methods which apply wave division multiplexing and demultiplexing for wireline communications as described in the preferred embodiments which pertain to FIGS. (14), (14′), and as referred to in the preferred embodiments which specifically include the application of relatively long wavelengths of electromagnetically neutralized quanta of electromagnetic radiation relative to optical wavelengths (which are referred to immediately following the preferred embodiment pertaining to FIG. 14′, and which are applicable to the preferred embodiment which pertains to FIG. 14), are, in general, applicable in the preferred embodiment for wireless communications illustrated in FIG. (16) with respective modifications including the application of only air (6 dk) as a coherent transmission medium instead of air filled tubing.

Wherein, in both preferred embodiments (15) and (16), the adverse electromagnetic interaction of the neutralized beam with electrically charged particles comprised in the air is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the coherently transmitted neutralized beam during transmission. In which case, the adverse electromagnetic effects of transmitting energy for wireless communications are eliminated to a directly proportional extent, e.g., signal attenuation is eliminated in direct proportion to the time-averaged energy flux density which is eliminated from the respectively applied beam of electromagnetically neutralized quanta of electromagnetic radiation during transmission so as to increase the distance a signal can travel without being amplified (or repeated), such that the need for relatively high transmitter power output and/or the need for signal amplification (or repeating) is eliminated to a directly proportional extent, and such that the bandwidth (in terms of frequencies) which is available for signal transmission is increased.

To broaden, the detailed description of the present invention herein describes a limited number of the embodiments of the present invention. Yet, various other embodiments of the present invention can be included in the scope of the present invention. Thus, the present invention should be interpreted in as broad a scope as possible so as to include all the equivalent embodiments of the present invention.

Notes: Reference characters (2), (4), (6), and (8) in the present patent disclosure each represent a parent part comprising the full scope of the group of parts which each have a reference character with the same number and a lower case letter (or letters) following the number, and each of these reference characters which are different from the parent part reference character represents a somewhat different scope (or selection) of the full set of versions of the parent part; Drawing, including drawing illustrating a beam of electromagnetically neutralized radiation, which is positioned inside other drawing is not illustrated as hidden, and thus, for example, a beam of electromagnetically neutralized radiation in such drawing is not represented by a dashed line. This is done in the case of a beam of electromagnetically neutralized radiation since the superposition resultant of a beam which is produced by complete destructive interference of forward traveling transverse waves and total cancellation of associated electromagnetic fields can be represented conventionally by a dashed line as illustrated in FIG. (2-a); Hatching which is applied to sectional views is somewhat generic in that it is not intended to represent any particular material, but rather it is intended to represent a range of materials relevant to the particular application; Thick dashed lines adjacent to hatched tubing is intended to indicated that the tubing extends farther than illustrated; The term “eliminate,” and each of the various forms thereof (including “eliminates,” “eliminated,” “eliminating,” and “elimination”) means to “omit” in its respective form in various forms of the phrases which relate to the time-averaged energy flux density which is eliminated from an electromagnetically neutralized beam, the elimination of adverse electromagnetic interaction, the elimination of adverse electromagnetic effects, and any similar phrase; The term “time-averaged energy flux density” means “intensity”; A photodetector and a particle detector are each defined as a radiation detector; The term “total destructive interference” should be considered as the maximum amount of destructive interference possible with respect to an electromagnetically neutralized beam of radiation, such that an electromagnetically neutralized beam of radiation produced with total destructive interference is considered an electromagnetically neutralized coherent beam of superimposed quasi-monoenergetic quanta of electromagnetic radiation, or an electromagnetically neutralized coherent beam of superimposed quasi-monoenergetic electrically charged particles. Wherein, all other related references such as a “superposition resultant of zero magnitude”; a “resultant electromagnetic field of zero magnitude”; a “time-averaged energy flux density of zero magnitude”; the total electromagnetic neutralization of a beam; “total electric charge neutralization”; “totally electromagnetically neutralized radiation”; the total elimination of time-averaged energy flux density from a beam; the total elimination of the adverse electromagnetic interaction of a neutralized beam with electrically charged particles in a coherent transmission medium; and the total elimination of the adverse electromagnetic effects of transmitting energy should be considered as approximations, which establish relative starting “zero” references accordingly. Wherein, an applied beam of totally electromagnetically neutralized radiation “minimally” electromagnetically interacts with, and “minimally” transfers energy to, electrically charged particles in transmission apparatus during coherent transmission; References to the amount of electromagnetic intensity comprised by a beam (or radiation comprised in a beam) pertain to the conditions of the waves and associated electromagnetic fields comprised by the beam. Wherein, for example, the term “partly electromagnetically intense” (or the like) with respect to a uniform beam of partly electromagnetically neutralized radiation pertains to the condition of the beam of partly neutralized radiation in that it comprises coherent radiation comprising superimposed forward traveling transverse waves which not only partly destructively interfere, but also partly constructively interfere; and in that it comprises associated electromagnetic fields which not only partly cancel, but also partly reinforce. In which case, the beam of partly electromagnetically neutralized radiation is “partly electromagnetically intense” (i.e., comprises a partial intensity or a partial time-averaged energy flux density) relative to the maximum possible intensity comprised by a hypothetical beam of totally electromagnetically intense radiation which would be equivalent except that it would be produced with total constructive interference of respectively comprised waves, and total reinforcement of the respectively associated electromagnetic fields; or relative to the maximum possible intensity comprised by a hypothetical beam of totally electromagnetically intense radiation which would be equivalent except that it would be produced with total spatial incoherence. Wherein, it is considered that a uniform beam such as beam (4 b) and beam (4 h) (or radiation comprised in such a uniform beam) is electromagnetically intense relative to the maximum and minimum (i.e., “zero”) possible intensities of the beam of which it is comprised as relates to such hypothetical beams; Any reference to a beam comprising radiation which relates to a beam of electromagnetically neutralized radiation, is meant to include a quantum mechanically significantly large quantity of radiation en masse, or a quantum mechanically significantly large quantity of radiation over an extended interval of time; The elimination of the adverse electromagnetic interaction of a beam of electromagnetically neutralized radiation with electrically charged particles comprised in a coherent transmission apparatus in the present invention is based on the application of a beam of electromagnetically neutralized radiation of quantum mechanically significantly large quantities which is coherently transmitted en masse through electrically charged particles, or based on the application of any quantity of electromagnetically neutralized radiation which is coherently transmitted through a quantum mechanically significant length of electrically charged particles; Coherence length should be consider with respect to the maintenance and elimination of destructive interference of forward traveling transverse waves, and the maintenance and elimination of the cancellation of respectively associated electromagnetic fields of a beam of electromagnetically neutralized radiation applied in the present invention; Certain beams of radiation (e.g., one or more beams of radiation which are created by, for example, backscattering; backreflections; multiple reflections, e.g., secondary reflections; or extraneous beams; in any given embodiment in the specification herein may not be illustrated and/or may not be referred to in some way or ways so that any such embodiment of the present invention is not too confusing; The overall objective (or the overall effective result) of the present invention includes the objective of transmitting energy in order to accomplish a particular result, and also includes the objective of doing so in an efficient manner (i.e., doing so without an applied beam of electromagnetically neutralized radiation adversely electromagnetically interacting with, and transferring energy to, electrically charged particles comprised in a coherent transmission medium to an extent, and without related adverse electromagnetic effects to a directly proportional extent). 

I claim:
 1. A method of transmitting a beam of electromagnetically neutralized radiation for transmitting energy in an energy efficient manner, wherein the method comprises the steps of: 1) generating a beam of electromagnetically neutralized radiation by superimposing coherent forward traveling transverse waves in the beam an amount out of phase, wherein the radiation in the beam comprises forward propagating particles comprising at least one selected from the group of forward propagating photons and forward propagating electrically charged particles, wherein the particles are associated with the waves, and the displacement vectors of the waves in the beam cancel in direct proportion to the amount to which the waves are out of phase in order to produce a directly proportional amount of destructive interference which produces associated electric and magnetic field resultants which produce an intensity which is indirectly proportional to the amount of the destructive interference; and the method further comprising the steps of 2) coherently transmitting the radiation in the beam through electrically charged particles to a transducer, wherein as the beam is transmitted through the electrically charged particles the amount of energy transferred from the beam to the electrically charged particles by manner of electromagnetic interaction is indirectly proportional to the amount of the destructive interference, and directly proportional to the intensity of the resultant electromagnetic field, such that the interaction of the beam with the electrically charged particles is controlled by the intensity of the beam; and 3) transferring energy from the transmitted beam of electromagnetically neutralized radiation to the transducer, wherein the transmitted energy is transduced into a result by the transducer comprising at least one selected from the group of electrical voltage and electrical current.
 2. A method of transmitting a beam of electromagnetically neutralized radiation for transmitting energy in an energy efficient manner, wherein the method comprises the steps of: 1) providing a source of coherent radiation and interferometric apparatus for producing a beam of electromagnetically neutralized radiation by superimposing coherent forward traveling transverse waves in the beam an amount out of phase, wherein the radiation in the beam comprises forward propagating particles comprising at least one selected from the group of forward propagating photons and forward propagating electrically charged particles, wherein the particles are associated with the waves, and the displacement vectors of the waves in the beam cancel in direct proportion to the amount to which the waves are out of phase in order to produce a directly proportional amount of destructive interference which produces associated electric and magnetic field resultants which produce an intensity which is indirectly proportional to the amount of the destructive interference; and the method further comprising the steps of 2) coherently transmitting the radiation in the beam through electrically charged particles to a transducer, wherein as the beam is transmitted through the electrically charged particles the amount of energy transferred from the beam to the electrically charged particles by manner of electromagnetic interaction is indirectly proportional to the amount of the destructive interference, and directly proportional to the intensity of the resultant electromagnetic field, such that the interaction of the beam with the electrically charged particles is controlled by the intensity of the beam; and 3) transferring energy from the transmitted beam of electromagnetically neutralized radiation to the transducer, wherein the transmitted energy is transduced into a result by the transducer comprising at least one selected from the group of electrical voltage and electrical current.
 3. The method of claim 1, more specifically in which the beam of electromagnetically neutralized radiation comprises at least one change in the magnitude of momentum, and more specifically in which the transducer is a pressure transducer wherein at least one change of momentum comprised in the transmitted particle beam is applied upon the pressure transducer so that the pressure transducer produces the result which comprises at least one change in output comprising at least one selected from the group of electrical voltage output and electrical current output.
 4. The method of claim 3, more specifically in which the pressure transducer comprises a reflective surface, and further comprising the step of coherently reflecting the neutralized particle beam from the reflective surface of the pressure transducer, and further comprising at least one step selected from the group comprising the step of coherently transmitting the reflected particle beam to at least one other pressure transducer and the step of coherently reflecting the reflected particle beam back to the first pressure transducer, wherein the process is repeated in equivalent terms at least once, such that a plurality of changes in the same quality of outputs are produced.
 5. The method of claim 4, more specifically in which at least one property of the momentum comprised in the neutralized particle beam selected from the group of amplitude, frequency, and phase is modulated with a modulator in order to encode at least one datum, wherein the voltage which is produced with each pressure transducer encodes at least one datum which is available for retrieval during an interval of time.
 6. The method of claim 1, more specifically in which the beam of electromagnetically neutralized radiation comprises a beam of partly electromagnetically neutralized radiation comprising waves with an amount of partial destructive interference and partial constructive interference, and associated electric and magnetic fields which are each cancelled in direct proportion to the amount of the destructive interference and reinforced in direct proportion to the amount of the constructive interference, and more specifically in which the transducer is a radiation detector comprising electrically charged particles wherein energy is transferred from the transmitted beam of partly electromagnetically neutralized radiation to the electrically charged particles comprised in the target by manner of electromagnetic interaction in order to produce the result in the radiation detector.
 7. (canceled)
 8. A method of transmitting a beam of electromagnetically neutralized radiation for transmitting energy in an energy efficient manner, wherein the method comprises the steps of: 1) generating a beam of electromagnetically neutralized radiation by superimposing coherent forward traveling transverse waves in the beam an amount out of phase, wherein the radiation in the beam comprises forward propagating particles comprising at least one selected from the group of forward propagating photons and forward propagating electrically charged particles, wherein the particles are associated with the waves, and the displacement vectors of the waves in the beam cancel in direct proportion to the amount to which the waves are out of phase in order to produce a directly proportional amount of destructive interference which produces associated electric and magnetic field resultants which produce an intensity which is indirectly proportional to the amount of the destructive interference; and the method further comprising the steps of 2) coherently transmitting the radiation in the beam through electrically charged particles to a transducer, wherein as the beam is transmitted through the electrically charged particles the amount of energy transferred from the beam to the electrically charged particles by manner of electromagnetic interaction is indirectly proportional to the amount of the destructive interference, and directly proportional to the intensity of the resultant electromagnetic field, such that the interaction of the beam with the electrically charged particles is controlled by the intensity of the beam; 3) incoherently scattering an amount of the transmitted beam with apparatus in order to produce a resulting beam selected from the group of a beam of incoherent radiation and a beam of incoherent radiation in combination with a beam of electromagnetically neutralized radiation, wherein the scattering apparatus is comprised in the transducer, and wherein the amount of incoherent radiation in the resulting beam is based on the amount of the scattering of the transmitted neutralized beam; and 4) transferring energy from the resultant beam to the electrically charged particles comprised in the transducer by manner of electromagnetic interaction, wherein the transmitted energy is transduced into a result by the transducer comprising at least one selected from the group of electrical voltage and electrical current. 